Ajout licence CC By-Sa
This commit is contained in:
parent
3eaf5d98b9
commit
89ae7aa334
@ -1,18 +1,18 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {G}Chute de la Lune}{127}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {G}Chute de la Lune}{189}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{chutelunecirculaire}{{G}{127}}
|
\newlabel{chutelunecirculaire}{{G}{189}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {G.1}Introduction}{127}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {G.1}Introduction}{189}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {G.2}Acc\IeC {\'e}l\IeC {\'e}ration}{127}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {G.2}Acc\IeC {\'e}l\IeC {\'e}ration}{189}\protected@file@percent }
|
||||||
\newlabel{chutedelalune}{{G.2}{127}}
|
\newlabel{chutedelalune}{{G.2}{189}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {G.1}{\ignorespaces Chute de la lune\relax }}{127}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {G.1}{\ignorespaces Chute de la lune\relax }}{189}\protected@file@percent }
|
||||||
\newlabel{schemachutelune}{{G.1}{127}}
|
\newlabel{schemachutelune}{{G.1}{189}}
|
||||||
\newlabel{equation1}{{G.1}{128}}
|
\newlabel{equation1}{{G.1}{190}}
|
||||||
\newlabel{equation2}{{G.2}{128}}
|
\newlabel{equation2}{{G.2}{190}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {G.3}Force de gravitation}{128}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {G.3}Force de gravitation}{190}\protected@file@percent }
|
||||||
\@setckpt{Annexe-ChuteLune/Annexe-ChuteLune}{
|
\@setckpt{Annexe-ChuteLune/Annexe-ChuteLune}{
|
||||||
\setcounter{page}{129}
|
\setcounter{page}{191}
|
||||||
\setcounter{equation}{2}
|
\setcounter{equation}{2}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -34,7 +34,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -42,7 +42,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{58}
|
\setcounter{endnote}{64}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,24 +1,24 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {K}\IeC {\'E}nergies}{143}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {K}\IeC {\'E}nergies}{205}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {K.1}Introduction}{143}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {K.1}Introduction}{205}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {K.2}\IeC {\'E}nergie hydraulique}{143}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {K.2}\IeC {\'E}nergie hydraulique}{205}\protected@file@percent }
|
||||||
\newlabel{barrageduchatelot}{{K.2}{143}}
|
\newlabel{barrageduchatelot}{{K.2}{205}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {K.1}{\ignorespaces Le barrage du Ch\IeC {\^a}telot}}{143}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {K.1}{\ignorespaces Le barrage du Ch\IeC {\^a}telot}}{205}\protected@file@percent }
|
||||||
\newlabel{chatelot@ch\IeC {\^a}telot}{{K.1}{143}}
|
\newlabel{chatelot@ch\IeC {\^a}telot}{{K.1}{205}}
|
||||||
\newlabel{prodchatelot}{{K.1}{143}}
|
\newlabel{prodchatelot}{{K.1}{205}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {K.3}\IeC {\'E}nergie \IeC {\'e}olienne}{144}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {K.3}\IeC {\'E}nergie \IeC {\'e}olienne}{206}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {K.3.1}R\IeC {\`e}gle de Betz}{144}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {K.3.1}R\IeC {\`e}gle de Betz}{206}\protected@file@percent }
|
||||||
\newlabel{reglebetz}{{K.3.1}{144}}
|
\newlabel{reglebetz}{{K.3.1}{206}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {K.3.2}\IeC {\'E}oliennes}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {K.3.2}\IeC {\'E}oliennes}{207}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}olienne de Collonges-Dor\IeC {\'e}naz}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}olienne de Collonges-Dor\IeC {\'e}naz}{207}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}oliennes du Mont Soleil (Jura suisse)}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}oliennes du Mont Soleil (Jura suisse)}{207}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {K.4}G\IeC {\'e}othermie}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {K.4}G\IeC {\'e}othermie}{207}\protected@file@percent }
|
||||||
\newlabel{riehen}{{K.4}{145}}
|
\newlabel{riehen}{{K.4}{207}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {K.5}\IeC {\'E}nergie de combustion des d\IeC {\'e}chets}{146}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {K.5}\IeC {\'E}nergie de combustion des d\IeC {\'e}chets}{208}\protected@file@percent }
|
||||||
\@setckpt{Annexe-Energies/Annexe-Energies}{
|
\@setckpt{Annexe-Energies/Annexe-Energies}{
|
||||||
\setcounter{page}{147}
|
\setcounter{page}{209}
|
||||||
\setcounter{equation}{3}
|
\setcounter{equation}{3}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -40,7 +40,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -48,7 +48,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{65}
|
\setcounter{endnote}{71}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
222304
Annexe-Energies/Images/ChatelotConduiteForcee.eps
Normal file
222304
Annexe-Energies/Images/ChatelotConduiteForcee.eps
Normal file
File diff suppressed because it is too large
Load Diff
BIN
Annexe-Energies/Images/ChatelotConduiteForcee.jpg
Normal file
BIN
Annexe-Energies/Images/ChatelotConduiteForcee.jpg
Normal file
Binary file not shown.
|
After Width: | Height: | Size: 3.4 MiB |
19823
Annexe-Energies/Images/ChatelotConduiteForceeCoupe.eps
Normal file
19823
Annexe-Energies/Images/ChatelotConduiteForceeCoupe.eps
Normal file
File diff suppressed because it is too large
Load Diff
BIN
Annexe-Energies/Images/ChatelotConduiteForceeCoupe.jpg
Normal file
BIN
Annexe-Energies/Images/ChatelotConduiteForceeCoupe.jpg
Normal file
Binary file not shown.
|
After Width: | Height: | Size: 227 KiB |
114286
Annexe-Energies/Images/ChatelotTurbines.eps
Normal file
114286
Annexe-Energies/Images/ChatelotTurbines.eps
Normal file
File diff suppressed because it is too large
Load Diff
BIN
Annexe-Energies/Images/ChatelotTurbines.jpg
Normal file
BIN
Annexe-Energies/Images/ChatelotTurbines.jpg
Normal file
Binary file not shown.
|
After Width: | Height: | Size: 1.9 MiB |
@ -1,50 +1,74 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {L}Exercices}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {L}Exercices}{209}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{exos}{{L}{147}}
|
\newlabel{exos}{{L}{209}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {L.1}Probl\IeC {\`e}mes}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {L.1}Probl\IeC {\`e}mes}{209}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.1}Relatifs \IeC {\`a} la conversion d'unit\IeC {\'e}s et \IeC {\`a} la notation scientifique}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.1}Relatifs \IeC {\`a} la conversion d'unit\IeC {\'e}s et \IeC {\`a} la notation scientifique}{209}\protected@file@percent }
|
||||||
\newlabel{centaure}{{1}{147}}
|
\newlabel{centaure}{{1}{209}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.2}Relatifs aux notions de d\IeC {\'e}placement, position et distance parcourue}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.2}Relatifs aux notions de d\IeC {\'e}placement, position et distance parcourue}{209}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.1}{\ignorespaces Le rayon de la Terre par Eratosth\IeC {\`e}ne\relax }}{148}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.1}{\ignorespaces Le rayon de la Terre par Eratosth\IeC {\`e}ne\relax }}{210}\protected@file@percent }
|
||||||
\newlabel{Erathostene}{{L.1}{148}}
|
\newlabel{Erathostene}{{L.1}{210}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.3}Relatifs \IeC {\`a} la notion de vitesse}{148}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.3}Relatifs \IeC {\`a} la notion de vitesse}{210}\protected@file@percent }
|
||||||
\newlabel{vitrotterresoleil}{{15}{148}}
|
\newlabel{vitrotterresoleil}{{15}{210}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.4}Relatif \IeC {\`a} la notion d'acc\IeC {\'e}l\IeC {\'e}ration}{148}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.4}Relatif \IeC {\`a} la notion d'acc\IeC {\'e}l\IeC {\'e}ration}{210}\protected@file@percent }
|
||||||
\newlabel{vitsprinter}{{18}{148}}
|
\newlabel{vitsprinter}{{18}{210}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.5}Relatif au MRU}{149}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.5}Relatif au MRU}{211}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.6}Relatif au MRUA}{149}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.6}Relatif au MRUA}{211}\protected@file@percent }
|
||||||
\newlabel{caspremier}{{1}{149}}
|
\newlabel{caspremier}{{1}{211}}
|
||||||
\newlabel{castroisieme}{{3}{149}}
|
\newlabel{castroisieme}{{3}{211}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.7}Relatifs \IeC {\`a} la physique aristot\IeC {\'e}licienne}{150}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.7}Relatifs \IeC {\`a} la physique aristot\IeC {\'e}licienne}{212}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.8}Relatifs \IeC {\`a} la physique newtonienne}{150}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.8}Relatifs \IeC {\`a} la physique newtonienne}{212}\protected@file@percent }
|
||||||
\newlabel{exfusee}{{36}{151}}
|
\newlabel{exfusee}{{36}{213}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.2}{\ignorespaces La poulie}}{151}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.2}{\ignorespaces La poulie}}{213}\protected@file@percent }
|
||||||
\newlabel{poulie}{{L.2}{151}}
|
\newlabel{poulie}{{L.2}{213}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.9}Relatifs aux forces}{151}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.3}{\ignorespaces Masse pendante}}{214}\protected@file@percent }
|
||||||
\newlabel{massedelaterre}{{48}{152}}
|
\newlabel{pendante}{{L.3}{214}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.10}Relatifs \IeC {\`a} l'\IeC {\'e}nergie}{152}\protected@file@percent }
|
\newlabel{planinclinesimple}{{4}{214}}
|
||||||
\newlabel{helico}{{54}{152}}
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.4}{\ignorespaces Deux poulies}}{214}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.11}Relatifs \IeC {\`a} la conservation de l'\IeC {\'e}nergie}{152}\protected@file@percent }
|
\newlabel{deuxpoulies}{{L.4}{214}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.12}Relatifs \IeC {\`a} l'\IeC {\'e}nergie hydraulique}{153}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.9}Relatifs aux forces}{214}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.13}Relatifs \IeC {\`a} l'\IeC {\'e}nergie \IeC {\'e}olienne}{153}\protected@file@percent }
|
\newlabel{massedelaterre}{{48}{215}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.14}Relatifs \IeC {\`a} l'\IeC {\'e}nergie solaire}{153}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.5}{\ignorespaces Bloc suspendu}}{216}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {L.2}Solutions}{154}\protected@file@percent }
|
\newlabel{blocsuspendu}{{L.5}{216}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.3}{\ignorespaces Graphes horaires du MRU.\relax }}{157}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.10}Relatifs \IeC {\`a} l'\IeC {\'e}nergie}{216}\protected@file@percent }
|
||||||
\newlabel{graphesmru}{{L.3}{157}}
|
\newlabel{helico}{{54}{216}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.4}{\ignorespaces Chute aristot\IeC {\'e}licienne de la tour Eiffel.\relax }}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.11}Relatifs \IeC {\`a} la conservation de l'\IeC {\'e}nergie}{216}\protected@file@percent }
|
||||||
\newlabel{eiffelmecanique}{{L.4}{160}}
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.12}Relatifs \IeC {\`a} l'\IeC {\'e}nergie hydraulique}{217}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.5}{\ignorespaces Une fus\IeC {\'e}e.\relax }}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.13}Relatifs \IeC {\`a} l'\IeC {\'e}nergie \IeC {\'e}olienne}{217}\protected@file@percent }
|
||||||
\newlabel{fusee}{{L.5}{160}}
|
\@writefile{toc}{\contentsline {subsection}{\numberline {L.1.14}Relatifs \IeC {\`a} l'\IeC {\'e}nergie solaire}{217}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.6}{\ignorespaces Une remorque\relax }}{161}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {L.2}Solutions}{218}\protected@file@percent }
|
||||||
\newlabel{remorque}{{L.6}{161}}
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.6}{\ignorespaces Graphes horaires du MRU.\relax }}{221}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {L.7}{\ignorespaces Un ascenseur\relax }}{164}\protected@file@percent }
|
\newlabel{graphesmru}{{L.6}{221}}
|
||||||
\newlabel{ascenseur}{{L.7}{164}}
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.7}{\ignorespaces Chute aristot\IeC {\'e}licienne de la tour Eiffel.\relax }}{224}\protected@file@percent }
|
||||||
|
\newlabel{eiffelmecanique}{{L.7}{224}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.8}{\ignorespaces Une fus\IeC {\'e}e.\relax }}{224}\protected@file@percent }
|
||||||
|
\newlabel{fusee}{{L.8}{224}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.9}{\ignorespaces Une remorque\relax }}{225}\protected@file@percent }
|
||||||
|
\newlabel{remorque}{{L.9}{225}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.10}{\ignorespaces Un ascenseur\relax }}{228}\protected@file@percent }
|
||||||
|
\newlabel{ascenseur}{{L.10}{228}}
|
||||||
|
\@writefile{toc}{\contentsline {section}{\numberline {L.3}Solutions OS}{233}\protected@file@percent }
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.11}{\ignorespaces Force inclin\IeC {\'e}e}}{233}\protected@file@percent }
|
||||||
|
\newlabel{forceinclinee}{{L.11}{233}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.12}{\ignorespaces Lampe suspendue}}{234}\protected@file@percent }
|
||||||
|
\newlabel{lampe}{{L.12}{234}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.13}{\ignorespaces Plan inclin\IeC {\'e}}}{235}\protected@file@percent }
|
||||||
|
\newlabel{incline}{{L.13}{235}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.14}{\ignorespaces Corde poulie}}{238}\protected@file@percent }
|
||||||
|
\newlabel{cordepoulie}{{L.14}{238}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.15}{\ignorespaces Corde tir\IeC {\'e}e poulie}}{238}\protected@file@percent }
|
||||||
|
\newlabel{cordepoulietiree}{{L.15}{238}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.16}{\ignorespaces Corde tir\IeC {\'e}e poulie juste}}{238}\protected@file@percent }
|
||||||
|
\newlabel{cordepoulietireejuste}{{L.16}{238}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.17}{\ignorespaces Frottements}}{241}\protected@file@percent }
|
||||||
|
\newlabel{inclinefrottement}{{L.17}{241}}
|
||||||
|
\@writefile{lof}{\contentsline {figure}{\numberline {L.18}{\ignorespaces Forces sur bloc suspendu}}{242}\protected@file@percent }
|
||||||
|
\newlabel{blocsuspenduforces}{{L.18}{242}}
|
||||||
\@setckpt{Annexe-Exercices/Annexe-Exercices}{
|
\@setckpt{Annexe-Exercices/Annexe-Exercices}{
|
||||||
\setcounter{page}{170}
|
\setcounter{page}{244}
|
||||||
\setcounter{equation}{0}
|
\setcounter{equation}{0}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
\setcounter{enumiii}{0}
|
\setcounter{enumiii}{0}
|
||||||
\setcounter{enumiv}{0}
|
\setcounter{enumiv}{0}
|
||||||
@ -52,19 +76,19 @@
|
|||||||
\setcounter{mpfootnote}{0}
|
\setcounter{mpfootnote}{0}
|
||||||
\setcounter{part}{0}
|
\setcounter{part}{0}
|
||||||
\setcounter{chapter}{12}
|
\setcounter{chapter}{12}
|
||||||
\setcounter{section}{2}
|
\setcounter{section}{3}
|
||||||
\setcounter{subsection}{0}
|
\setcounter{subsection}{0}
|
||||||
\setcounter{subsubsection}{0}
|
\setcounter{subsubsection}{0}
|
||||||
\setcounter{paragraph}{0}
|
\setcounter{paragraph}{0}
|
||||||
\setcounter{subparagraph}{0}
|
\setcounter{subparagraph}{0}
|
||||||
\setcounter{figure}{7}
|
\setcounter{figure}{18}
|
||||||
\setcounter{table}{0}
|
\setcounter{table}{0}
|
||||||
\setcounter{NAT@ctr}{0}
|
\setcounter{NAT@ctr}{0}
|
||||||
\setcounter{FBcaption@count}{0}
|
\setcounter{FBcaption@count}{0}
|
||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -72,7 +96,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{66}
|
\setcounter{endnote}{72}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
@ -81,7 +105,7 @@
|
|||||||
\setcounter{lstnumber}{1}
|
\setcounter{lstnumber}{1}
|
||||||
\setcounter{Solution}{71}
|
\setcounter{Solution}{71}
|
||||||
\setcounter{exc}{71}
|
\setcounter{exc}{71}
|
||||||
\setcounter{Solution OS}{0}
|
\setcounter{Solution OS}{20}
|
||||||
\setcounter{exosc}{0}
|
\setcounter{exosc}{20}
|
||||||
\setcounter{lstlisting}{0}
|
\setcounter{lstlisting}{0}
|
||||||
}
|
}
|
||||||
|
|||||||
@ -1,28 +1,28 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {M}Ordre de grandeur, erreur et incertitudes}{249}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {M}Ordre de grandeur, erreur et incertitudes}{245}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {M.1}Ordre de grandeur}{249}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {M.1}Ordre de grandeur}{245}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.1.1}Chiffres significatifs}{249}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.1.1}Chiffres significatifs}{245}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.1.2}Ordre de grandeur}{249}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.1.2}Ordre de grandeur}{245}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {M.2}\IeC {\'E}cart et erreur}{250}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {M.2}\IeC {\'E}cart et erreur}{246}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {M.1}{\ignorespaces La longueur des baguettes de pain\relax }}{250}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {M.1}{\ignorespaces La longueur des baguettes de pain\relax }}{246}\protected@file@percent }
|
||||||
\newlabel{baguettepain}{{M.1}{250}}
|
\newlabel{baguettepain}{{M.1}{246}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {M.2}{\ignorespaces La longueur d'autres baguettes de pain\relax }}{251}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {M.2}{\ignorespaces La longueur d'autres baguettes de pain\relax }}{247}\protected@file@percent }
|
||||||
\newlabel{baguettepain2}{{M.2}{251}}
|
\newlabel{baguettepain2}{{M.2}{247}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {M.3}{\ignorespaces Des centaines de baguettes de pain\relax }}{251}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {M.3}{\ignorespaces Des centaines de baguettes de pain\relax }}{247}\protected@file@percent }
|
||||||
\newlabel{enclassementbaguettes}{{M.3}{251}}
|
\newlabel{enclassementbaguettes}{{M.3}{247}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {M.1}{\ignorespaces Baguettes d'une ann\IeC {\'e}e\relax }}{252}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {M.1}{\ignorespaces Baguettes d'une ann\IeC {\'e}e\relax }}{248}\protected@file@percent }
|
||||||
\newlabel{baguettesgauss}{{M.1}{252}}
|
\newlabel{baguettesgauss}{{M.1}{248}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {M.3}Incertitude}{252}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {M.3}Incertitude}{248}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.1}Addition/soustraction}{252}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.1}Addition/soustraction}{248}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.2}Multiplication par un entier}{253}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.2}Multiplication par un entier}{249}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.3}Multiplication/division}{253}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.3}Multiplication/division}{249}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.4}Puissance}{254}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.4}Puissance}{250}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.5}R\IeC {\'e}sum\IeC {\'e}}{254}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.5}R\IeC {\'e}sum\IeC {\'e}}{250}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.6}Exemples}{255}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {M.3.6}Exemples}{251}\protected@file@percent }
|
||||||
\@setckpt{Annexe-Incertitudes/Annexe-Incertitudes}{
|
\@setckpt{Annexe-Incertitudes/Annexe-Incertitudes}{
|
||||||
\setcounter{page}{256}
|
\setcounter{page}{252}
|
||||||
\setcounter{equation}{1}
|
\setcounter{equation}{1}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,19 +1,19 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {F}MRUA d\IeC {\'e}veloppements}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {F}MRUA d\IeC {\'e}veloppements}{187}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {F.1}La position}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {F.1}La position}{187}\protected@file@percent }
|
||||||
\newlabel{demo}{{F.1}{125}}
|
\newlabel{demo}{{F.1}{187}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {F.1}{\ignorespaces \emph {Discours concernant deux sciences nouvelles} de Galil\IeC {\'e}e}}{125}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {F.1}{\ignorespaces \emph {Discours concernant deux sciences nouvelles} de Galil\IeC {\'e}e}}{187}\protected@file@percent }
|
||||||
\newlabel{deuxsciences}{{F.1}{125}}
|
\newlabel{deuxsciences}{{F.1}{187}}
|
||||||
\newlabel{pratique}{{F.2}{125}}
|
\newlabel{pratique}{{F.2}{187}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {F.2}Une autre relation bien pratique}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {F.2}Une autre relation bien pratique}{187}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {F.2.1}Cin\IeC {\'e}matique}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {F.2.1}Cin\IeC {\'e}matique}{187}\protected@file@percent }
|
||||||
\newlabel{sanst}{{F.2}{126}}
|
\newlabel{sanst}{{F.2}{188}}
|
||||||
\newlabel{demo2}{{F.2.1}{126}}
|
\newlabel{demo2}{{F.2.1}{188}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {F.2.2}\IeC {\'E}nergie}{126}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {F.2.2}\IeC {\'E}nergie}{188}\protected@file@percent }
|
||||||
\@setckpt{Annexe-MRUA/Annexe-MRUA}{
|
\@setckpt{Annexe-MRUA/Annexe-MRUA}{
|
||||||
\setcounter{page}{127}
|
\setcounter{page}{189}
|
||||||
\setcounter{equation}{2}
|
\setcounter{equation}{2}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -35,7 +35,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -43,7 +43,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{58}
|
\setcounter{endnote}{64}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,51 +1,51 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.1}{\ignorespaces Mar\IeC {\'e}e}}{135}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.1}{\ignorespaces Mar\IeC {\'e}e}}{197}\protected@file@percent }
|
||||||
\newlabel{maree}{{J.1}{135}}
|
\newlabel{maree}{{J.1}{197}}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {J}Mar\IeC {\'e}es}{135}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {J}Mar\IeC {\'e}es}{197}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{chapmarees}{{J}{135}}
|
\newlabel{chapmarees}{{J}{197}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.1}Introduction}{135}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.1}Introduction}{197}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.2}Centre de gravit\IeC {\'e}}{135}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.2}Centre de gravit\IeC {\'e}}{197}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.2}{\ignorespaces Syst\IeC {\`e}me Terre-Lune\relax }}{136}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.2}{\ignorespaces Syst\IeC {\`e}me Terre-Lune\relax }}{198}\protected@file@percent }
|
||||||
\newlabel{systterrelune}{{J.2}{136}}
|
\newlabel{systterrelune}{{J.2}{198}}
|
||||||
\newlabel{distgrav}{{J.1}{136}}
|
\newlabel{distgrav}{{J.1}{198}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.3}Force d'inertie}{136}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.3}Force d'inertie}{198}\protected@file@percent }
|
||||||
\newlabel{acccentr}{{J.2}{136}}
|
\newlabel{acccentr}{{J.2}{198}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.3.1}Vitesse angulaire}{136}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.3.1}Vitesse angulaire}{198}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.3}{\ignorespaces Syst\IeC {\`e}me Terre-Lune-eau\relax }}{136}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.3}{\ignorespaces Syst\IeC {\`e}me Terre-Lune-eau\relax }}{198}\protected@file@percent }
|
||||||
\newlabel{systterreluneeau}{{J.3}{136}}
|
\newlabel{systterreluneeau}{{J.3}{198}}
|
||||||
\newlabel{omega}{{J.3}{136}}
|
\newlabel{omega}{{J.3}{198}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.3.2}Force d'inertie}{136}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.3.2}Force d'inertie}{198}\protected@file@percent }
|
||||||
\newlabel{forceinertie}{{J.4}{136}}
|
\newlabel{forceinertie}{{J.4}{198}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.4}Poids relatif}{137}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.4}Poids relatif}{199}\protected@file@percent }
|
||||||
\newlabel{Newacc}{{J.5}{137}}
|
\newlabel{Newacc}{{J.5}{199}}
|
||||||
\newlabel{DLmaree}{{J.6}{137}}
|
\newlabel{DLmaree}{{J.6}{199}}
|
||||||
\newlabel{secondeloimaree}{{J.7}{137}}
|
\newlabel{secondeloimaree}{{J.7}{199}}
|
||||||
\newlabel{forcedemareebalance}{{J.8}{137}}
|
\newlabel{forcedemareebalance}{{J.8}{199}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.5}Analyse diff\IeC {\'e}rentielle}{137}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.5}Analyse diff\IeC {\'e}rentielle}{199}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.6}Autres rythmes}{137}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.6}Autres rythmes}{199}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.4}{\ignorespaces D\IeC {\'e}calage horaire}}{138}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.4}{\ignorespaces D\IeC {\'e}calage horaire}}{200}\protected@file@percent }
|
||||||
\newlabel{decalage}{{J.4}{138}}
|
\newlabel{decalage}{{J.4}{200}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.1}D\IeC {\'e}calages}{138}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.1}D\IeC {\'e}calages}{200}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.2}Mar\IeC {\'e}es de vives et mortes eaux}{138}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.2}Mar\IeC {\'e}es de vives et mortes eaux}{200}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.5}{\ignorespaces Vives et mortes eaux}}{138}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.5}{\ignorespaces Vives et mortes eaux}}{200}\protected@file@percent }
|
||||||
\newlabel{vivemorteeau}{{J.5}{138}}
|
\newlabel{vivemorteeau}{{J.5}{200}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.3}Mar\IeC {\'e}es d'\IeC {\'e}quinoxes}{138}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.3}Mar\IeC {\'e}es d'\IeC {\'e}quinoxes}{200}\protected@file@percent }
|
||||||
\citation{BS07}
|
\citation{BS07}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.4}Mar\IeC {\'e}es de p\IeC {\'e}rig\IeC {\'e}e et p\IeC {\'e}rih\IeC {\'e}lie}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.4}Mar\IeC {\'e}es de p\IeC {\'e}rig\IeC {\'e}e et p\IeC {\'e}rih\IeC {\'e}lie}{201}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.5}Mar\IeC {\'e}es de d\IeC {\'e}clinaison}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.5}Mar\IeC {\'e}es de d\IeC {\'e}clinaison}{201}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.6}Retards et mar\IeC {\'e}es c\IeC {\^o}ti\IeC {\`e}res}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.6.6}Retards et mar\IeC {\'e}es c\IeC {\^o}ti\IeC {\`e}res}{201}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {J.7}Limite de Roche}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {J.7}Limite de Roche}{201}\protected@file@percent }
|
||||||
\newlabel{limroche}{{J.7}{139}}
|
\newlabel{limroche}{{J.7}{201}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.6}{\ignorespaces Limite de Roche}}{140}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.6}{\ignorespaces Limite de Roche}}{202}\protected@file@percent }
|
||||||
\newlabel{roche}{{J.6}{140}}
|
\newlabel{roche}{{J.6}{202}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.7.1}Mod\IeC {\`e}le simplifi\IeC {\'e}}{140}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.7.1}Mod\IeC {\`e}le simplifi\IeC {\'e}}{202}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {J.7}{\ignorespaces Limite de Roche}}{141}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {J.7}{\ignorespaces Limite de Roche}}{203}\protected@file@percent }
|
||||||
\newlabel{limitederoche}{{J.7}{141}}
|
\newlabel{limitederoche}{{J.7}{203}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {J.7.2}Exemples}{141}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {J.7.2}Exemples}{203}\protected@file@percent }
|
||||||
\@setckpt{Annexe-Maree/Annexe-Maree}{
|
\@setckpt{Annexe-Maree/Annexe-Maree}{
|
||||||
\setcounter{page}{142}
|
\setcounter{page}{204}
|
||||||
\setcounter{equation}{10}
|
\setcounter{equation}{10}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -67,7 +67,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -75,7 +75,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{61}
|
\setcounter{endnote}{67}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,32 +1,32 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {C}Mesures de distances}{105}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {C}Mesures de distances}{167}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {C.1}La taille de la Terre}{105}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {C.1}La taille de la Terre}{167}\protected@file@percent }
|
||||||
\newlabel{tailleterre}{{C.1}{105}}
|
\newlabel{tailleterre}{{C.1}{167}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {C.1.1}Le principe}{105}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {C.1.1}Le principe}{167}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {C.1}{\ignorespaces Taille de la terre\relax }}{105}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {C.1}{\ignorespaces Taille de la terre\relax }}{167}\protected@file@percent }
|
||||||
\newlabel{erathostenetailleterre}{{C.1}{105}}
|
\newlabel{erathostenetailleterre}{{C.1}{167}}
|
||||||
\citation{AS02}
|
\citation{AS02}
|
||||||
\citation{JJD21}
|
\citation{JJD21}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {C.1.2}Techniquement}{106}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {C.1.2}Techniquement}{168}\protected@file@percent }
|
||||||
\newlabel{scaphe}{{a}{106}}
|
\newlabel{scaphe}{{a}{168}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {C.2}La taille de la Lune}{107}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {C.2}La taille de la Lune}{169}\protected@file@percent }
|
||||||
\newlabel{taillelune}{{C.2}{107}}
|
\newlabel{taillelune}{{C.2}{169}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {C.2}{\ignorespaces Taille de la lune}}{107}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {C.2}{\ignorespaces Taille de la lune}}{169}\protected@file@percent }
|
||||||
\newlabel{tailledelalune}{{C.2}{107}}
|
\newlabel{tailledelalune}{{C.2}{169}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {C.3}La distance Terre-Lune}{107}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {C.3}La distance Terre-Lune}{169}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {C.4}La distance Terre-Soleil}{108}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {C.4}La distance Terre-Soleil}{170}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {C.3}{\ignorespaces Parallaxe de Mars}}{108}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {C.3}{\ignorespaces Parallaxe de Mars}}{170}\protected@file@percent }
|
||||||
\newlabel{parallaxemars}{{C.3}{108}}
|
\newlabel{parallaxemars}{{C.3}{170}}
|
||||||
\newlabel{dtm}{{C.1}{109}}
|
\newlabel{dtm}{{C.1}{171}}
|
||||||
\newlabel{opposition}{{C.2}{109}}
|
\newlabel{opposition}{{C.2}{171}}
|
||||||
\newlabel{oppositionkepler}{{C.3}{109}}
|
\newlabel{oppositionkepler}{{C.3}{171}}
|
||||||
\newlabel{cassiniua}{{C.4}{109}}
|
\newlabel{cassiniua}{{C.4}{171}}
|
||||||
\newlabel{cassiniuaexcentrique}{{C.5}{110}}
|
\newlabel{cassiniuaexcentrique}{{C.5}{172}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {C.5}La distance des \IeC {\'e}toiles}{110}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {C.5}La distance des \IeC {\'e}toiles}{172}\protected@file@percent }
|
||||||
\@setckpt{Annexe-MesuresDistances/Annexe-MesuresDistances}{
|
\@setckpt{Annexe-MesuresDistances/Annexe-MesuresDistances}{
|
||||||
\setcounter{page}{111}
|
\setcounter{page}{173}
|
||||||
\setcounter{equation}{5}
|
\setcounter{equation}{5}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -48,7 +48,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -56,7 +56,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{54}
|
\setcounter{endnote}{60}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,31 +1,31 @@
|
|||||||
\relax
|
\relax
|
||||||
\citation{GC88}
|
\citation{GC88}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {I}Relativit\IeC {\'e}}{131}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {I}Relativit\IeC {\'e}}{193}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{relativite}{{I}{131}}
|
\newlabel{relativite}{{I}{193}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {I.1}Relativit\IeC {\'e} galil\IeC {\'e}enne}{131}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {I.1}Relativit\IeC {\'e} galil\IeC {\'e}enne}{193}\protected@file@percent }
|
||||||
\citation{JR00}
|
\citation{JR00}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {I.2}Transformation galil\IeC {\'e}enne}{132}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {I.2}Transformation galil\IeC {\'e}enne}{194}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {I.1}{\ignorespaces Transformation de galil\IeC {\'e}e}}{132}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {I.1}{\ignorespaces Transformation de galil\IeC {\'e}e}}{194}\protected@file@percent }
|
||||||
\newlabel{transgalilee}{{I.1}{132}}
|
\newlabel{transgalilee}{{I.1}{194}}
|
||||||
\newlabel{eqtransgalilee}{{I.1}{132}}
|
\newlabel{eqtransgalilee}{{I.1}{194}}
|
||||||
\newlabel{thmaddvit}{{I.2}{132}}
|
\newlabel{thmaddvit}{{I.2}{194}}
|
||||||
\citation{GC88}
|
\citation{GC88}
|
||||||
\newlabel{thmaddvit2}{{I.3}{133}}
|
\newlabel{thmaddvit2}{{I.3}{195}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {I.3}Invariance}{133}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {I.3}Invariance}{195}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {I.4}Forces inertielles}{133}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {I.4}Forces inertielles}{195}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {I.4.1}Force d'inertie}{133}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {I.4.1}Force d'inertie}{195}\protected@file@percent }
|
||||||
\citation{GC88}
|
\citation{GC88}
|
||||||
\newlabel{accobjetdsreftournant}{{I.5}{134}}
|
\newlabel{accobjetdsreftournant}{{I.5}{196}}
|
||||||
\newlabel{accreftournant}{{I.6}{134}}
|
\newlabel{accreftournant}{{I.6}{196}}
|
||||||
\newlabel{acctournantfinale}{{I.7}{134}}
|
\newlabel{acctournantfinale}{{I.7}{196}}
|
||||||
\newlabel{secondeR}{{I.8}{134}}
|
\newlabel{secondeR}{{I.8}{196}}
|
||||||
\newlabel{secondeR'}{{I.9}{134}}
|
\newlabel{secondeR'}{{I.9}{196}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {I.4.2}Force centrifuge}{134}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {I.4.2}Force centrifuge}{196}\protected@file@percent }
|
||||||
\newlabel{forcecentrifuge}{{I.4.2}{134}}
|
\newlabel{forcecentrifuge}{{I.4.2}{196}}
|
||||||
\@setckpt{Annexe-Relativite/Annexe-Relativite}{
|
\@setckpt{Annexe-Relativite/Annexe-Relativite}{
|
||||||
\setcounter{page}{135}
|
\setcounter{page}{197}
|
||||||
\setcounter{equation}{11}
|
\setcounter{equation}{11}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -47,7 +47,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -55,7 +55,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{59}
|
\setcounter{endnote}{65}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,19 +1,19 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {E}Rotations}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {E}Rotations}{183}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {E.1}Rotation de la Terre sur elle-m\IeC {\^e}me}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {E.1}Rotation de la Terre sur elle-m\IeC {\^e}me}{183}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {E.2}Rotation de la Terre autour du Soleil}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {E.2}Rotation de la Terre autour du Soleil}{183}\protected@file@percent }
|
||||||
\citation{GG92}
|
\citation{GG92}
|
||||||
\citation{JR07}
|
\citation{JR07}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {E.1}{\ignorespaces Le syst\IeC {\`e}me g\IeC {\'e}ocentrique de Tycho Brah\IeC {\'e}}}{122}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {E.1}{\ignorespaces Le syst\IeC {\`e}me g\IeC {\'e}ocentrique de Tycho Brah\IeC {\'e}}}{184}\protected@file@percent }
|
||||||
\newlabel{tychosystem}{{E.1}{122}}
|
\newlabel{tychosystem}{{E.1}{184}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {E.3}Rotation du Soleil dans la Voie Lact\IeC {\'e}e}{123}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {E.3}Rotation du Soleil dans la Voie Lact\IeC {\'e}e}{185}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {E.2}{\ignorespaces Le Soleil dans la Voie Lact\IeC {\'e}e}}{123}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {E.2}{\ignorespaces Le Soleil dans la Voie Lact\IeC {\'e}e}}{185}\protected@file@percent }
|
||||||
\newlabel{milky_way_2005}{{E.2}{123}}
|
\newlabel{milky_way_2005}{{E.2}{185}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {E.4}Vitesse et r\IeC {\'e}f\IeC {\'e}rentiel}{123}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {E.4}Vitesse et r\IeC {\'e}f\IeC {\'e}rentiel}{185}\protected@file@percent }
|
||||||
\@setckpt{Annexe-Rotations/Annexe-Rotations}{
|
\@setckpt{Annexe-Rotations/Annexe-Rotations}{
|
||||||
\setcounter{page}{125}
|
\setcounter{page}{187}
|
||||||
\setcounter{equation}{0}
|
\setcounter{equation}{0}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -35,7 +35,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -43,7 +43,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{57}
|
\setcounter{endnote}{63}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,18 +1,18 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {H}Satellite en orbite g\IeC {\'e}ostationnaire}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {H}Satellite en orbite g\IeC {\'e}ostationnaire}{191}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{geostat}{{H}{129}}
|
\newlabel{geostat}{{H}{191}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {H.1}Introduction}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {H.1}Introduction}{191}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {H.2}Th\IeC {\'e}oriquement}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {H.2}Th\IeC {\'e}oriquement}{191}\protected@file@percent }
|
||||||
\newlabel{vitessesatgeostat}{{H.1}{129}}
|
\newlabel{vitessesatgeostat}{{H.1}{191}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {H.1}{\ignorespaces Satellite}}{129}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {H.1}{\ignorespaces Satellite}}{191}\protected@file@percent }
|
||||||
\newlabel{satellite}{{H.1}{129}}
|
\newlabel{satellite}{{H.1}{191}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {H.3}Num\IeC {\'e}riquement}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {H.3}Num\IeC {\'e}riquement}{192}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {H.4}Loi de Kepler}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {H.4}Loi de Kepler}{192}\protected@file@percent }
|
||||||
\newlabel{keplergeostat}{{H.4}{130}}
|
\newlabel{keplergeostat}{{H.4}{192}}
|
||||||
\@setckpt{Annexe-Satellites/Annexe-Satellites}{
|
\@setckpt{Annexe-Satellites/Annexe-Satellites}{
|
||||||
\setcounter{page}{131}
|
\setcounter{page}{193}
|
||||||
\setcounter{equation}{1}
|
\setcounter{equation}{1}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -34,7 +34,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -42,7 +42,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{59}
|
\setcounter{endnote}{65}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,25 +1,25 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {B}Deux syst\IeC {\`e}mes de coordonn\IeC {\'e}es}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {B}Deux syst\IeC {\`e}mes de coordonn\IeC {\'e}es}{165}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{coordonn\IeC {\'e}es}{{B}{103}}
|
\newlabel{coordonn\IeC {\'e}es}{{B}{165}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {B.1}Le syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {B.1}Le syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires}{165}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {B.1.1}Introduction}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {B.1.1}Introduction}{165}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {B.1.2}Description}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {B.1.2}Description}{165}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {B.1}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires\relax }}{103}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {B.1}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires\relax }}{165}\protected@file@percent }
|
||||||
\newlabel{circulaire}{{B.1}{103}}
|
\newlabel{circulaire}{{B.1}{165}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {B.2}Coordonn\IeC {\'e}es sph\IeC {\'e}riques}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {B.2}Coordonn\IeC {\'e}es sph\IeC {\'e}riques}{165}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.1}Introduction}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.1}Introduction}{165}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.2}Description}{103}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.2}Description}{165}\protected@file@percent }
|
||||||
\newlabel{sph\IeC {\`e}re}{{B.2.2}{104}}
|
\newlabel{sph\IeC {\`e}re}{{B.2.2}{166}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {B.2}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es sph\IeC {\'e}riques\relax }}{104}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {B.2}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es sph\IeC {\'e}riques\relax }}{166}\protected@file@percent }
|
||||||
\newlabel{sph\IeC {\`e}rique}{{B.2}{104}}
|
\newlabel{sph\IeC {\`e}rique}{{B.2}{166}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.3}Latitude et longitude}{104}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {B.2.3}Latitude et longitude}{166}\protected@file@percent }
|
||||||
\newlabel{latitude}{{B.2.3}{104}}
|
\newlabel{latitude}{{B.2.3}{166}}
|
||||||
\@setckpt{Annexe-SystemeCoordonnees/Annexe-SystemeCoordonnees}{
|
\@setckpt{Annexe-SystemeCoordonnees/Annexe-SystemeCoordonnees}{
|
||||||
\setcounter{page}{105}
|
\setcounter{page}{167}
|
||||||
\setcounter{equation}{0}
|
\setcounter{equation}{0}
|
||||||
\setcounter{enumi}{7}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
\setcounter{enumiii}{0}
|
\setcounter{enumiii}{0}
|
||||||
\setcounter{enumiv}{0}
|
\setcounter{enumiv}{0}
|
||||||
@ -39,7 +39,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -47,7 +47,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{51}
|
\setcounter{endnote}{57}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,55 +1,55 @@
|
|||||||
\relax
|
\relax
|
||||||
\citation{JL96}
|
\citation{JL96}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {D}Travaux pratiques}{111}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {D}Travaux pratiques}{173}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.1}Le rapport de laboratoire}{111}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.1}Le rapport de laboratoire}{173}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.1.1}Plan d'un rapport de travail pratique}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.1.1}Plan d'un rapport de travail pratique}{174}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Pr\IeC {\'e}liminaires}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Pr\IeC {\'e}liminaires}{174}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{R\IeC {\'e}sum\IeC {\'e}}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{R\IeC {\'e}sum\IeC {\'e}}{174}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{But}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{But}{174}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {D.1}{\ignorespaces Rail horizontal}}{112}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {D.1}{\ignorespaces Rail horizontal}}{174}\protected@file@percent }
|
||||||
\newlabel{railhorizontal}{{D.1}{112}}
|
\newlabel{railhorizontal}{{D.1}{174}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Th\IeC {\'e}orie}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Th\IeC {\'e}orie}{174}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Description de l'exp\IeC {\'e}rience}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Description de l'exp\IeC {\'e}rience}{174}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{R\IeC {\'e}sultats}{112}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{R\IeC {\'e}sultats}{174}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {D.2}{\ignorespaces Chute libre\relax }}{113}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {D.2}{\ignorespaces Chute libre\relax }}{175}\protected@file@percent }
|
||||||
\newlabel{explegraphe}{{D.2}{113}}
|
\newlabel{explegraphe}{{D.2}{175}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {D.1}{\ignorespaces Tableau de mesures\relax }}{113}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {D.1}{\ignorespaces Tableau de mesures\relax }}{175}\protected@file@percent }
|
||||||
\newlabel{tableau}{{D.1}{113}}
|
\newlabel{tableau}{{D.1}{175}}
|
||||||
\newlabel{defecart}{{D.1}{113}}
|
\newlabel{defecart}{{D.1}{175}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Discussion}{114}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Discussion}{176}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Conclusion}{114}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Conclusion}{176}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Annexes}{114}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Annexes}{176}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.2}La n\IeC {\'e}buleuse du Crabe}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.2}La n\IeC {\'e}buleuse du Crabe}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.1}Introduction}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.1}Introduction}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.2}But du travail pratique}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.2}But du travail pratique}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.3}Dispositif exp\IeC {\'e}rimental}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.3}Dispositif exp\IeC {\'e}rimental}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.4}Mesures}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.4}Mesures}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.5}R\IeC {\'e}sultats}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.5}R\IeC {\'e}sultats}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.6}Analyse}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.2.6}Analyse}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.3}Le pendule simple}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.3}Le pendule simple}{177}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.3.1}Les mesures}{115}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.3.1}Les mesures}{177}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {D.3}{\ignorespaces Une pendule\relax }}{116}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {D.3}{\ignorespaces Une pendule\relax }}{178}\protected@file@percent }
|
||||||
\newlabel{fig:lelapendule}{{D.3}{116}}
|
\newlabel{fig:lelapendule}{{D.3}{178}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.3.2}Organisation des donn\IeC {\'e}es et graphiques}{117}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.3.2}Organisation des donn\IeC {\'e}es et graphiques}{179}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.4}Mouvement simple~: MRU}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.4}Mouvement simple~: MRU}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.1}Les mesures}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.1}Les mesures}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.2}Organisation des donn\IeC {\'e}es et graphiques}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.2}Organisation des donn\IeC {\'e}es et graphiques}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.3}Analyse des r\IeC {\'e}sultats}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.4.3}Analyse des r\IeC {\'e}sultats}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.5}Mouvement simple~:\\MRUA}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.5}Mouvement simple~:\\MRUA}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.1}But}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.1}But}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.2}Th\IeC {\'e}orie}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.2}Th\IeC {\'e}orie}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.3}Les mesures}{118}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.3}Les mesures}{180}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.4}Organisation des donn\IeC {\'e}es et graphiques}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.4}Organisation des donn\IeC {\'e}es et graphiques}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.5}Galil\IeC {\'e}e et le plan inclin\IeC {\'e}}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.5.5}Galil\IeC {\'e}e et le plan inclin\IeC {\'e}}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.6}La chute libre}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.6}La chute libre}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.6.1}Cette exp\IeC {\'e}rience donnant lieu \IeC {\`a} un rapport not\IeC {\'e}, elle n'est pas d\IeC {\'e}crite.}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.6.1}Cette exp\IeC {\'e}rience donnant lieu \IeC {\`a} un rapport not\IeC {\'e}, elle n'est pas d\IeC {\'e}crite.}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {D.6.2}R\IeC {\'e}sultats}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {D.6.2}R\IeC {\'e}sultats}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.7}Le canon horizontal}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.7}Le canon horizontal}{181}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {D.8}Le chariot \IeC {\`a} masse pendante}{120}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {D.8}Le chariot \IeC {\`a} masse pendante}{182}\protected@file@percent }
|
||||||
\@setckpt{Annexe-TravauxPratiques/Annexe-TravauxPratiques}{
|
\@setckpt{Annexe-TravauxPratiques/Annexe-TravauxPratiques}{
|
||||||
\setcounter{page}{121}
|
\setcounter{page}{183}
|
||||||
\setcounter{equation}{1}
|
\setcounter{equation}{1}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -71,7 +71,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -79,7 +79,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{2}
|
\setcounter{caption@flags}{2}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{54}
|
\setcounter{endnote}{60}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,34 +1,34 @@
|
|||||||
\relax
|
\relax
|
||||||
\citation{AK05}
|
\citation{AK05}
|
||||||
\citation{AS06}
|
\citation{AS06}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {A}Syst\IeC {\`e}mes d'unit\IeC {\'e}s}{97}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {A}Syst\IeC {\`e}mes d'unit\IeC {\'e}s}{159}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{SI}{{A}{97}}
|
\newlabel{SI}{{A}{159}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.1}Introduction}{97}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.1}Introduction}{159}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.2}Op\IeC {\'e}rateur d'unit\IeC {\'e}s}{97}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.2}Op\IeC {\'e}rateur d'unit\IeC {\'e}s}{159}\protected@file@percent }
|
||||||
\newlabel{express_unite}{{A.1}{97}}
|
\newlabel{express_unite}{{A.1}{159}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.3}Analyse dimensionnelle}{98}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.3}Analyse dimensionnelle}{160}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.4}Les unit\IeC {\'e}s du Syst\IeC {\`e}me International}{99}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.4}Les unit\IeC {\'e}s du Syst\IeC {\`e}me International}{161}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {A.4.1}Exemple}{99}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {A.4.1}Exemple}{161}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.5}Conversions}{99}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.5}Conversions}{161}\protected@file@percent }
|
||||||
\newlabel{relationdarc}{{A.2}{99}}
|
\newlabel{relationdarc}{{A.2}{161}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {A.1}{\ignorespaces Relation de l'arc de cercle\relax }}{99}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {A.1}{\ignorespaces Relation de l'arc de cercle\relax }}{161}\protected@file@percent }
|
||||||
\newlabel{arc}{{A.1}{99}}
|
\newlabel{arc}{{A.1}{161}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {A.1}{\ignorespaces Les unit\IeC {\'e}s du Syst\IeC {\`e}me International\relax }}{100}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {A.1}{\ignorespaces Les unit\IeC {\'e}s du Syst\IeC {\`e}me International\relax }}{162}\protected@file@percent }
|
||||||
\newlabel{AL}{{A.1}{100}}
|
\newlabel{AL}{{A.1}{162}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {A.2}{\ignorespaces Conversions d'unit\IeC {\'e}s\relax }}{100}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {A.2}{\ignorespaces Conversions d'unit\IeC {\'e}s\relax }}{162}\protected@file@percent }
|
||||||
\newlabel{grandeurs}{{A.2}{100}}
|
\newlabel{grandeurs}{{A.2}{162}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.6}Sous-multiples}{100}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.6}Sous-multiples}{162}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {A.3}{\ignorespaces Quelques \IeC {\'e}quivalents\relax }}{100}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {A.3}{\ignorespaces Quelques \IeC {\'e}quivalents\relax }}{162}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.7}Notation scientifique}{100}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.7}Notation scientifique}{162}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {A.4}{\ignorespaces Multiples et sous-multiples\relax }}{101}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {A.4}{\ignorespaces Multiples et sous-multiples\relax }}{163}\protected@file@percent }
|
||||||
\newlabel{prefixes}{{A.4}{101}}
|
\newlabel{prefixes}{{A.4}{163}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {A.8}R\IeC {\`e}gles de calcul}{101}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {A.8}R\IeC {\`e}gles de calcul}{163}\protected@file@percent }
|
||||||
\@setckpt{Annexe-UnitesInternationales/Annexe-UnitesInternationales}{
|
\@setckpt{Annexe-UnitesInternationales/Annexe-UnitesInternationales}{
|
||||||
\setcounter{page}{102}
|
\setcounter{page}{164}
|
||||||
\setcounter{equation}{2}
|
\setcounter{equation}{2}
|
||||||
\setcounter{enumi}{7}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
\setcounter{enumiii}{0}
|
\setcounter{enumiii}{0}
|
||||||
\setcounter{enumiv}{0}
|
\setcounter{enumiv}{0}
|
||||||
@ -48,7 +48,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -56,7 +56,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{0}
|
\setcounter{caption@flags}{0}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{51}
|
\setcounter{endnote}{57}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,95 +1,95 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {2}La cin\IeC {\'e}matique}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {2}La cin\IeC {\'e}matique}{33}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {2.1}Introduction}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {2.1}Introduction}{33}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {2.2}Position}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {2.2}Position}{33}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.1}Dimensions}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.1}Dimensions}{33}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.2}Syst\IeC {\`e}me d'axes}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.2}Syst\IeC {\`e}me d'axes}{33}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.1}{\ignorespaces Un syst\IeC {\`e}me d'axes en une dimension\relax }}{37}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.1}{\ignorespaces Un syst\IeC {\`e}me d'axes en une dimension\relax }}{33}\protected@file@percent }
|
||||||
\newlabel{1dim}{{2.1}{37}}
|
\newlabel{1dim}{{2.1}{33}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.3}Position}{37}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.3}Position}{33}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.2}{\ignorespaces La position d'un objet\relax }}{38}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.2}{\ignorespaces La position d'un objet\relax }}{34}\protected@file@percent }
|
||||||
\newlabel{position}{{2.2}{38}}
|
\newlabel{position}{{2.2}{34}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.4}D\IeC {\'e}placement}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.4}D\IeC {\'e}placement}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.5}Distance parcourue}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.5}Distance parcourue}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {2.3}Vitesse}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {2.3}Vitesse}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.1}Vitesse moyenne}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.1}Vitesse moyenne}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.2}Exemples}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.2}Exemples}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemple 1}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemple 1}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemple 2}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemple 2}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.3}Vitesse instantan\IeC {\'e}e}{38}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3.3}Vitesse instantan\IeC {\'e}e}{34}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {2.4}Acc\IeC {\'e}l\IeC {\'e}ration}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {2.4}Acc\IeC {\'e}l\IeC {\'e}ration}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.1}Acc\IeC {\'e}l\IeC {\'e}ration moyenne}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.1}Acc\IeC {\'e}l\IeC {\'e}ration moyenne}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.2}Exemples}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.2}Exemples}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemple 1}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemple 1}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemple 2}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemple 2}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Remarque~:}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Remarque~:}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.3}L'acc\IeC {\'e}l\IeC {\'e}ration instantan\IeC {\'e}e}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.4.3}L'acc\IeC {\'e}l\IeC {\'e}ration instantan\IeC {\'e}e}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {2.5}Mouvements simples}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {2.5}Mouvements simples}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.1}Le mouvement rectiligne uniforme}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.1}Le mouvement rectiligne uniforme}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{35}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{39}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{35}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.3}{\ignorespaces Apollo 16}}{40}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.3}{\ignorespaces Apollo 16}}{36}\protected@file@percent }
|
||||||
\newlabel{apollo16}{{2.3}{40}}
|
\newlabel{apollo16}{{2.3}{36}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Un exemple~: Apollo en route vers la Lune}{40}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Un exemple~: Apollo en route vers la Lune}{36}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {2.1}{\ignorespaces Donn\IeC {\'e}es de la mission Apollo 12\relax }}{40}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {2.1}{\ignorespaces Donn\IeC {\'e}es de la mission Apollo 12\relax }}{36}\protected@file@percent }
|
||||||
\newlabel{donneesdapollo}{{2.1}{40}}
|
\newlabel{donneesdapollo}{{2.1}{36}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.4}{\ignorespaces Collision Androm\IeC {\`e}de-Voie Lact\IeC {\'e}e}}{41}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.4}{\ignorespaces Collision Androm\IeC {\`e}de-Voie Lact\IeC {\'e}e}}{37}\protected@file@percent }
|
||||||
\newlabel{andromede_collision}{{2.4}{41}}
|
\newlabel{andromede_collision}{{2.4}{37}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Autre exemple~: le d\IeC {\'e}placement d'Androm\IeC {\`e}de}{41}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Autre exemple~: le d\IeC {\'e}placement d'Androm\IeC {\`e}de}{37}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.2}Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e} (MRUA)}{41}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.2}Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e} (MRUA)}{37}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{41}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{37}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{41}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{37}\protected@file@percent }
|
||||||
\citation{SH03}
|
\citation{SH03}
|
||||||
\citation{SH03}
|
\citation{SH03}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.3}La chute libre}{42}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.3}La chute libre}{38}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {2.2}{\ignorespaces La hauteur en fonction du temps\relax }}{42}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {2.2}{\ignorespaces La hauteur en fonction du temps\relax }}{38}\protected@file@percent }
|
||||||
\newlabel{brutes}{{2.2}{42}}
|
\newlabel{brutes}{{2.2}{38}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}finition}{42}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}finition}{38}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{42}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{38}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Exp\IeC {\'e}rience}{42}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Exp\IeC {\'e}rience}{38}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Calculs}{42}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Calculs}{38}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {2.3}{\ignorespaces La vitesse en fonction du temps\relax }}{43}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {2.3}{\ignorespaces La vitesse en fonction du temps\relax }}{39}\protected@file@percent }
|
||||||
\newlabel{vitesse}{{2.3}{43}}
|
\newlabel{vitesse}{{2.3}{39}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Analyse des r\IeC {\'e}sultats}{43}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Analyse des r\IeC {\'e}sultats}{39}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.5}{\ignorespaces Chute libre\relax }}{44}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.5}{\ignorespaces Chute libre\relax }}{40}\protected@file@percent }
|
||||||
\newlabel{graphehauteur}{{2.5}{44}}
|
\newlabel{graphehauteur}{{2.5}{40}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.6}{\ignorespaces Chute libre\relax }}{44}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.6}{\ignorespaces Chute libre\relax }}{40}\protected@file@percent }
|
||||||
\newlabel{graphevitesse}{{2.6}{44}}
|
\newlabel{graphevitesse}{{2.6}{40}}
|
||||||
\newlabel{accg}{{2.5.3}{44}}
|
\newlabel{accg}{{2.5.3}{40}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Conclusions}{44}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Conclusions}{40}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.4}Balistique}{44}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.4}Balistique}{40}\protected@file@percent }
|
||||||
\newlabel{balistique}{{2.5.4}{44}}
|
\newlabel{balistique}{{2.5.4}{40}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}finition}{44}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}finition}{40}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{44}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{40}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{\IeC {\'E}quations}{44}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{\IeC {\'E}quations}{40}\protected@file@percent }
|
||||||
\citation{EL99}
|
\citation{EL99}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Premier exemple}{45}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Premier exemple}{41}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Second exemple}{45}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Second exemple}{41}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.5}La chute libre ... de la Lune}{45}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.5}La chute libre ... de la Lune}{41}\protected@file@percent }
|
||||||
\newlabel{chutelibredelalune}{{2.5.5}{45}}
|
\newlabel{chutelibredelalune}{{2.5.5}{41}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.7}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune\relax }}{46}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.7}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune\relax }}{42}\protected@file@percent }
|
||||||
\newlabel{chutelune}{{2.7}{46}}
|
\newlabel{chutelune}{{2.7}{42}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.8}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{46}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.8}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{42}\protected@file@percent }
|
||||||
\newlabel{chutelunenewton}{{2.8}{46}}
|
\newlabel{chutelunenewton}{{2.8}{42}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.9}{\ignorespaces Chute de la Lune sur la Terre\relax }}{46}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.9}{\ignorespaces Chute de la Lune sur la Terre\relax }}{42}\protected@file@percent }
|
||||||
\newlabel{quartchutelune}{{2.9}{46}}
|
\newlabel{quartchutelune}{{2.9}{42}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.6}Mouvement circulaire uniforme (MCU)}{47}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.6}Mouvement circulaire uniforme (MCU)}{43}\protected@file@percent }
|
||||||
\newlabel{MvtCU}{{2.5.6}{47}}
|
\newlabel{MvtCU}{{2.5.6}{43}}
|
||||||
\newlabel{vomegar}{{2.13}{47}}
|
\newlabel{vomegar}{{2.13}{43}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Relation importante}{47}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Relation importante}{43}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.10}{\ignorespaces Mouvement circulaire uniforme\relax }}{48}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.10}{\ignorespaces Mouvement circulaire uniforme\relax }}{44}\protected@file@percent }
|
||||||
\newlabel{MCU}{{2.10}{48}}
|
\newlabel{MCU}{{2.10}{44}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.7}Lois de Kepler}{48}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {2.5.7}Lois de Kepler}{44}\protected@file@percent }
|
||||||
\newlabel{loiskepler}{{2.5.7}{48}}
|
\newlabel{loiskepler}{{2.5.7}{44}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.11}{\ignorespaces Astronomica pars Optica}}{49}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.11}{\ignorespaces Astronomica pars Optica}}{45}\protected@file@percent }
|
||||||
\newlabel{oeil}{{2.11}{49}}
|
\newlabel{oeil}{{2.11}{45}}
|
||||||
\newlabel{keplertroisieme}{{2.16}{49}}
|
\newlabel{keplertroisieme}{{2.16}{45}}
|
||||||
\newlabel{RF1}{50}
|
\newlabel{RF1}{46}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {2.12}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de cin\IeC {\'e}matique\relax }}{50}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {2.12}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de cin\IeC {\'e}matique\relax }}{46}\protected@file@percent }
|
||||||
\@setckpt{Cinematique/Cinematique}{
|
\@setckpt{Cinematique/Cinematique}{
|
||||||
\setcounter{page}{51}
|
\setcounter{page}{47}
|
||||||
\setcounter{equation}{24}
|
\setcounter{equation}{24}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
Binary file not shown.
Binary file not shown.
@ -8,8 +8,14 @@
|
|||||||
\@input{Introduction/Introduction.aux}
|
\@input{Introduction/Introduction.aux}
|
||||||
\@input{Cinematique/Cinematique.aux}
|
\@input{Cinematique/Cinematique.aux}
|
||||||
\@input{Dynamique/Dynamique.aux}
|
\@input{Dynamique/Dynamique.aux}
|
||||||
|
\@input{MecaniqueDim/MecaniqueDim.aux}
|
||||||
|
\@input{MecaniqueDifferentielle/MecaniqueDifferentielle.aux}
|
||||||
|
\@input{QtiteMvt/QtiteMvt.aux}
|
||||||
\@input{Energie/Energie.aux}
|
\@input{Energie/Energie.aux}
|
||||||
|
\@input{EnergieOS/EnergieOS.aux}
|
||||||
|
\@input{PhysiqueTheorique/PhysiqueTheorique.aux}
|
||||||
\@input{Thermodynamique/Thermodynamique.aux}
|
\@input{Thermodynamique/Thermodynamique.aux}
|
||||||
|
\@input{ThermodynamiqueOS/ThermodynamiqueOS.aux}
|
||||||
\@input{Annexe-UnitesInternationales/Annexe-UnitesInternationales.aux}
|
\@input{Annexe-UnitesInternationales/Annexe-UnitesInternationales.aux}
|
||||||
\@input{Annexe-SystemeCoordonnees/Annexe-SystemeCoordonnees.aux}
|
\@input{Annexe-SystemeCoordonnees/Annexe-SystemeCoordonnees.aux}
|
||||||
\@input{Annexe-MesuresDistances/Annexe-MesuresDistances.aux}
|
\@input{Annexe-MesuresDistances/Annexe-MesuresDistances.aux}
|
||||||
@ -22,6 +28,7 @@
|
|||||||
\@input{Annexe-Maree/Annexe-Maree.aux}
|
\@input{Annexe-Maree/Annexe-Maree.aux}
|
||||||
\@input{Annexe-Energies/Annexe-Energies.aux}
|
\@input{Annexe-Energies/Annexe-Energies.aux}
|
||||||
\@input{Annexe-Exercices/Annexe-Exercices.aux}
|
\@input{Annexe-Exercices/Annexe-Exercices.aux}
|
||||||
|
\@input{Annexe-Incertitudes/Annexe-Incertitudes.aux}
|
||||||
\bibstyle{apalike-fr}
|
\bibstyle{apalike-fr}
|
||||||
\bibdata{Bibliographies/BiblioCours}
|
\bibdata{Bibliographies/BiblioCours}
|
||||||
\bibcite{AK05}{{1}{2005}{{Alder}}{{}}}
|
\bibcite{AK05}{{1}{2005}{{Alder}}{{}}}
|
||||||
|
|||||||
Binary file not shown.
@ -466,14 +466,27 @@ Wikipedia~:
|
|||||||
=http://commons.wikimedia.org/wiki/Image:Rollercoaster_Tornado_Avonturenpark_Hellendoorn_Netherlands.jpg=
|
=http://commons.wikimedia.org/wiki/Image:Rollercoaster_Tornado_Avonturenpark_Hellendoorn_Netherlands.jpg=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {39}
|
\@doanenote {39}
|
||||||
macro:->Voir
|
macro:->Une
|
||||||
le
|
excellente
|
||||||
site
|
analyse
|
||||||
|
du
|
||||||
|
choc
|
||||||
de
|
de
|
||||||
l'encyclopédie
|
deux
|
||||||
Wikipedia~:
|
disques
|
||||||
|
à
|
||||||
|
été
|
||||||
|
faite
|
||||||
|
par
|
||||||
|
Pascal
|
||||||
|
Rebetez
|
||||||
|
et
|
||||||
|
se
|
||||||
|
trouve
|
||||||
|
à
|
||||||
|
l'adresse
|
||||||
\url
|
\url
|
||||||
=http://commons.wikimedia.org/wiki/Image:Finowkanal-treidel.jpg=
|
{http://owl-ge.ch/IMG/pdf/choc_2D_avec_citation.pdf}
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {40}
|
\@doanenote {40}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
@ -483,16 +496,26 @@ de
|
|||||||
l'encyclopédie
|
l'encyclopédie
|
||||||
Wikipedia~:
|
Wikipedia~:
|
||||||
\url
|
\url
|
||||||
=http://commons.wikimedia.org/wiki/Image:Mozaic-garden009.jpg=
|
=http://commons.wikimedia.org/wiki/Image:Finowkanal-treidel.jpg=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {41}
|
\@doanenote {41}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
|
site
|
||||||
|
de
|
||||||
|
l'encyclopédie
|
||||||
|
Wikipedia~:
|
||||||
|
\url
|
||||||
|
=http://commons.wikimedia.org/wiki/Image:Mozaic-garden009.jpg=
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {42}
|
||||||
|
macro:->Voir
|
||||||
|
le
|
||||||
site~:
|
site~:
|
||||||
\url
|
\url
|
||||||
=http://www.emosson-lac.ch/barrage.htm=
|
=http://www.emosson-lac.ch/barrage.htm=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {42}
|
\@doanenote {43}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -502,7 +525,7 @@ Wikipedia~:
|
|||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:S_vs_pelton_schnitt_1_zoom.png=
|
=http://fr.wikipedia.org/wiki/Image:S_vs_pelton_schnitt_1_zoom.png=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {43}
|
\@doanenote {44}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -511,7 +534,7 @@ l'encyclopédie~:
|
|||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:Photoelectric_effect.png=
|
=http://fr.wikipedia.org/wiki/Image:Photoelectric_effect.png=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {44}
|
\@doanenote {45}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -520,7 +543,7 @@ l'encyclopédie~:
|
|||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:4inch_poly_solar_cell.jpg=
|
=http://fr.wikipedia.org/wiki/Image:4inch_poly_solar_cell.jpg=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {45}
|
\@doanenote {46}
|
||||||
macro:->voir
|
macro:->voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -528,7 +551,7 @@ OutilsSolaires~:
|
|||||||
\url
|
\url
|
||||||
=http://www.outilssolaires.com/pv/prin-bilan.htm=
|
=http://www.outilssolaires.com/pv/prin-bilan.htm=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {46}
|
\@doanenote {47}
|
||||||
macro:->voir
|
macro:->voir
|
||||||
aussi
|
aussi
|
||||||
l'étude~:
|
l'étude~:
|
||||||
@ -551,7 +574,7 @@ l'adresse~:
|
|||||||
\url
|
\url
|
||||||
=http://www.eupvplatform.org/fileadmin/Documents/Brochure-indicateurs_26_pays.pdf=
|
=http://www.eupvplatform.org/fileadmin/Documents/Brochure-indicateurs_26_pays.pdf=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {47}
|
\@doanenote {48}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -560,7 +583,7 @@ l'encyclopédie~:
|
|||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:Tableau-lindal.jpg=
|
=http://fr.wikipedia.org/wiki/Image:Tableau-lindal.jpg=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {48}
|
\@doanenote {49}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -569,7 +592,7 @@ l'encyclopédie~:
|
|||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:Boiling_nuclear_reactor.png=
|
=http://fr.wikipedia.org/wiki/Image:Boiling_nuclear_reactor.png=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {49}
|
\@doanenote {50}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -578,7 +601,28 @@ l'encyclopédie~:
|
|||||||
\url
|
\url
|
||||||
=http://commons.wikimedia.org/wiki/Image:Combustion_methane.png=
|
=http://commons.wikimedia.org/wiki/Image:Combustion_methane.png=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {50}
|
\@doanenote {51}
|
||||||
|
macro:->Voir
|
||||||
|
Wikipedia
|
||||||
|
:
|
||||||
|
\url
|
||||||
|
|https://fr.wikipedia.org/wiki/Principe_de_moindre_action|
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {52}
|
||||||
|
macro:->Voir
|
||||||
|
Wikipedia
|
||||||
|
:
|
||||||
|
\url
|
||||||
|
{https://fr.wikipedia.org/wiki/Principe_de_moindre_action_et_mécanique_classique}
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {53}
|
||||||
|
macro:->Voir
|
||||||
|
Wikipedia
|
||||||
|
:
|
||||||
|
\url
|
||||||
|
{https://fr.wikipedia.org/wiki/Principe_de_moindre_action_et_mécanique_classique}
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {54}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -603,12 +647,26 @@ pour
|
|||||||
le
|
le
|
||||||
copyright.
|
copyright.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {51}
|
\@doanenote {55}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
\url
|
\url
|
||||||
=http://fr.wikipedia.org/wiki/Image:Sadi_Carnot.jpeg=
|
=http://fr.wikipedia.org/wiki/Image:Sadi_Carnot.jpeg=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {52}
|
\@doanenote {56}
|
||||||
|
macro:->Voir
|
||||||
|
le
|
||||||
|
site
|
||||||
|
de
|
||||||
|
l'encyclopédie~:\\
|
||||||
|
http://fr.wikipedia.org/wiki/Masse\_atomique
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {57}
|
||||||
|
macro:->Voir
|
||||||
|
Wikipedia~:
|
||||||
|
\url
|
||||||
|
=http://fr.wikipedia.org/wiki/Fichier:4-Stroke-Engine.gif=
|
||||||
|
\@endanenote
|
||||||
|
\@doanenote {58}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -630,15 +688,15 @@ auteur
|
|||||||
Luc
|
Luc
|
||||||
Viatour.
|
Viatour.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {53}
|
\@doanenote {59}
|
||||||
macro:->\url
|
macro:->\url
|
||||||
=http://www.iap.fr/InformationCommunication/ArticlesGrandPublic/Etoiles/Transit/transit_parallaxe_mars_1672.html=
|
=http://www.iap.fr/InformationCommunication/ArticlesGrandPublic/Etoiles/Transit/transit_parallaxe_mars_1672.html=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {54}
|
\@doanenote {60}
|
||||||
macro:->\url
|
macro:->\url
|
||||||
=http://www.iap.fr/InformationCommunication/ArticlesGrandPublic/Etoiles/Transit/transit_parallaxe_mars_1672.html=
|
=http://www.iap.fr/InformationCommunication/ArticlesGrandPublic/Etoiles/Transit/transit_parallaxe_mars_1672.html=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {55}
|
\@doanenote {61}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -654,7 +712,7 @@ copyright
|
|||||||
de
|
de
|
||||||
l'image.
|
l'image.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {56}
|
\@doanenote {62}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -673,14 +731,14 @@ Remerciements
|
|||||||
la
|
la
|
||||||
NASA.
|
NASA.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {57}
|
\@doanenote {63}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
\url
|
\url
|
||||||
=http://www.dil.univ-mrs.fr/~gispert/enseignement/astronomie/5eme_partie/voieLactee.php=
|
=http://www.dil.univ-mrs.fr/~gispert/enseignement/astronomie/5eme_partie/voieLactee.php=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {58}
|
\@doanenote {64}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -690,7 +748,7 @@ Wikipedia~:
|
|||||||
\url
|
\url
|
||||||
=http://commons.wikimedia.org/wiki/Image:Galileo_Galilei\%2C_Discorsi_e_Dimostrazioni_Matematiche_Intorno_a_Due_Nuove_Scienze\%2C_1638_\%281400x1400\%29.png=.
|
=http://commons.wikimedia.org/wiki/Image:Galileo_Galilei\%2C_Discorsi_e_Dimostrazioni_Matematiche_Intorno_a_Due_Nuove_Scienze\%2C_1638_\%281400x1400\%29.png=.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {59}
|
\@doanenote {65}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -710,7 +768,7 @@ Remerciements
|
|||||||
la
|
la
|
||||||
NASA.
|
NASA.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {60}
|
\@doanenote {66}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -732,7 +790,7 @@ auteur
|
|||||||
Samuel
|
Samuel
|
||||||
Wantman.
|
Wantman.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {61}
|
\@doanenote {67}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -748,7 +806,7 @@ copyright
|
|||||||
de
|
de
|
||||||
l'image.
|
l'image.
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {62}
|
\@doanenote {68}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -757,7 +815,7 @@ RhônEole~:
|
|||||||
\url
|
\url
|
||||||
=http://www.rhoneole.ch/=
|
=http://www.rhoneole.ch/=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {63}
|
\@doanenote {69}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
le
|
le
|
||||||
site
|
site
|
||||||
@ -766,7 +824,7 @@ Juvent~:
|
|||||||
\url
|
\url
|
||||||
=http://www.juvent.ch/=
|
=http://www.juvent.ch/=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {64}
|
\@doanenote {70}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
les
|
les
|
||||||
sites
|
sites
|
||||||
@ -778,7 +836,7 @@ et
|
|||||||
\url
|
\url
|
||||||
=http://www.ader.ch/energieaufutur/energies/geothermie/index2.php=
|
=http://www.ader.ch/energieaufutur/energies/geothermie/index2.php=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {65}
|
\@doanenote {71}
|
||||||
macro:->voir
|
macro:->voir
|
||||||
dépliant
|
dépliant
|
||||||
``Nos
|
``Nos
|
||||||
@ -792,7 +850,7 @@ site~:
|
|||||||
\url
|
\url
|
||||||
=http://www.cridor.ch/content/doc/brochures.php=
|
=http://www.cridor.ch/content/doc/brochures.php=
|
||||||
\@endanenote
|
\@endanenote
|
||||||
\@doanenote {66}
|
\@doanenote {72}
|
||||||
macro:->Voir
|
macro:->Voir
|
||||||
l'article
|
l'article
|
||||||
complet
|
complet
|
||||||
|
|||||||
0
CoursMecaniqueOSDF.gnuploterrors
Normal file
0
CoursMecaniqueOSDF.gnuploterrors
Normal file
File diff suppressed because it is too large
Load Diff
@ -1,125 +1,195 @@
|
|||||||
\babel@toc {french}{}
|
\babel@toc {french}{}
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {1.1}{\ignorespaces L'univers profond}}{22}%
|
\contentsline {figure}{\numberline {1.1}{\ignorespaces L'univers profond}}{18}%
|
||||||
\contentsline {figure}{\numberline {1.2}{\ignorespaces Mod\IeC {\`e}les de courbure}}{22}%
|
\contentsline {figure}{\numberline {1.2}{\ignorespaces Mod\IeC {\`e}les de courbure}}{18}%
|
||||||
\contentsline {figure}{\numberline {1.3}{\ignorespaces L'\IeC {\'e}volution du Soleil}}{23}%
|
\contentsline {figure}{\numberline {1.3}{\ignorespaces L'\IeC {\'e}volution du Soleil}}{19}%
|
||||||
\contentsline {figure}{\numberline {1.4}{\ignorespaces Groupe local}}{24}%
|
\contentsline {figure}{\numberline {1.4}{\ignorespaces Groupe local}}{20}%
|
||||||
\contentsline {figure}{\numberline {1.5}{\ignorespaces Galaxie du Sombrero}}{24}%
|
\contentsline {figure}{\numberline {1.5}{\ignorespaces Galaxie du Sombrero}}{20}%
|
||||||
\contentsline {figure}{\numberline {1.6}{\ignorespaces Interaction de deux galaxies}}{25}%
|
\contentsline {figure}{\numberline {1.6}{\ignorespaces Interaction de deux galaxies}}{21}%
|
||||||
\contentsline {figure}{\numberline {1.7}{\ignorespaces N\IeC {\'e}buleuse plan\IeC {\'e}taire}}{25}%
|
\contentsline {figure}{\numberline {1.7}{\ignorespaces N\IeC {\'e}buleuse plan\IeC {\'e}taire}}{21}%
|
||||||
\contentsline {figure}{\numberline {1.8}{\ignorespaces Premi\IeC {\`e}re exoplan\IeC {\`e}te}}{25}%
|
\contentsline {figure}{\numberline {1.8}{\ignorespaces Premi\IeC {\`e}re exoplan\IeC {\`e}te}}{21}%
|
||||||
\contentsline {figure}{\numberline {1.9}{\ignorespaces Syst\IeC {\`e}me solaire}}{27}%
|
\contentsline {figure}{\numberline {1.9}{\ignorespaces Syst\IeC {\`e}me solaire}}{23}%
|
||||||
\contentsline {figure}{\numberline {1.10}{\ignorespaces La taille des plan\IeC {\`e}tes}}{28}%
|
\contentsline {figure}{\numberline {1.10}{\ignorespaces La taille des plan\IeC {\`e}tes}}{24}%
|
||||||
\contentsline {figure}{\numberline {1.11}{\ignorespaces La taille des plan\IeC {\`e}tes}}{29}%
|
\contentsline {figure}{\numberline {1.11}{\ignorespaces La taille des plan\IeC {\`e}tes}}{25}%
|
||||||
\contentsline {figure}{\numberline {1.12}{\ignorespaces Une com\IeC {\`e}te}}{29}%
|
\contentsline {figure}{\numberline {1.12}{\ignorespaces Une com\IeC {\`e}te}}{25}%
|
||||||
\contentsline {figure}{\numberline {1.13}{\ignorespaces \IeC {\'E}toiles filantes}}{29}%
|
\contentsline {figure}{\numberline {1.13}{\ignorespaces \IeC {\'E}toiles filantes}}{25}%
|
||||||
\contentsline {figure}{\numberline {1.14}{\ignorespaces Les saisons}}{30}%
|
\contentsline {figure}{\numberline {1.14}{\ignorespaces Les saisons}}{26}%
|
||||||
\contentsline {figure}{\numberline {1.15}{\ignorespaces Les saisons}}{30}%
|
\contentsline {figure}{\numberline {1.15}{\ignorespaces Les saisons}}{26}%
|
||||||
\contentsline {figure}{\numberline {1.16}{\ignorespaces La terre et la lune}}{30}%
|
\contentsline {figure}{\numberline {1.16}{\ignorespaces La terre et la lune}}{26}%
|
||||||
\contentsline {figure}{\numberline {1.17}{\ignorespaces Les phases de la lune}}{31}%
|
\contentsline {figure}{\numberline {1.17}{\ignorespaces Les phases de la lune}}{27}%
|
||||||
\contentsline {figure}{\numberline {1.18}{\ignorespaces Orbites de la lune et du soleil}}{31}%
|
\contentsline {figure}{\numberline {1.18}{\ignorespaces Orbites de la lune et du soleil}}{27}%
|
||||||
\contentsline {figure}{\numberline {1.19}{\ignorespaces Les mar\IeC {\'e}es\relax }}{32}%
|
\contentsline {figure}{\numberline {1.19}{\ignorespaces Les mar\IeC {\'e}es\relax }}{28}%
|
||||||
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Sans rotation de la lune}}}{32}%
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Sans rotation de la lune}}}{28}%
|
||||||
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Avec rotation de la lune}}}{32}%
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Avec rotation de la lune}}}{28}%
|
||||||
\contentsline {figure}{\numberline {1.20}{\ignorespaces La n\IeC {\'e}buleuse du Crabe}}{32}%
|
\contentsline {figure}{\numberline {1.20}{\ignorespaces La n\IeC {\'e}buleuse du Crabe}}{28}%
|
||||||
\contentsline {figure}{\numberline {1.21}{\ignorespaces L'atome de Bohr}}{33}%
|
\contentsline {figure}{\numberline {1.21}{\ignorespaces L'atome de Bohr}}{29}%
|
||||||
\contentsline {figure}{\numberline {1.22}{\ignorespaces L'atome~: onde de probabilit\IeC {\'e}}}{35}%
|
\contentsline {figure}{\numberline {1.22}{\ignorespaces L'atome~: onde de probabilit\IeC {\'e}}}{31}%
|
||||||
\contentsline {figure}{\numberline {1.23}{\ignorespaces L'orbitale~: onde de probabilit\IeC {\'e}}}{35}%
|
\contentsline {figure}{\numberline {1.23}{\ignorespaces L'orbitale~: onde de probabilit\IeC {\'e}}}{31}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {2.1}{\ignorespaces Un syst\IeC {\`e}me d'axes en une dimension\relax }}{37}%
|
\contentsline {figure}{\numberline {2.1}{\ignorespaces Un syst\IeC {\`e}me d'axes en une dimension\relax }}{33}%
|
||||||
\contentsline {figure}{\numberline {2.2}{\ignorespaces La position d'un objet\relax }}{38}%
|
\contentsline {figure}{\numberline {2.2}{\ignorespaces La position d'un objet\relax }}{34}%
|
||||||
\contentsline {figure}{\numberline {2.3}{\ignorespaces Apollo 16}}{40}%
|
\contentsline {figure}{\numberline {2.3}{\ignorespaces Apollo 16}}{36}%
|
||||||
\contentsline {figure}{\numberline {2.4}{\ignorespaces Collision Androm\IeC {\`e}de-Voie Lact\IeC {\'e}e}}{41}%
|
\contentsline {figure}{\numberline {2.4}{\ignorespaces Collision Androm\IeC {\`e}de-Voie Lact\IeC {\'e}e}}{37}%
|
||||||
\contentsline {figure}{\numberline {2.5}{\ignorespaces Chute libre\relax }}{44}%
|
\contentsline {figure}{\numberline {2.5}{\ignorespaces Chute libre\relax }}{40}%
|
||||||
\contentsline {figure}{\numberline {2.6}{\ignorespaces Chute libre\relax }}{44}%
|
\contentsline {figure}{\numberline {2.6}{\ignorespaces Chute libre\relax }}{40}%
|
||||||
\contentsline {figure}{\numberline {2.7}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune\relax }}{46}%
|
\contentsline {figure}{\numberline {2.7}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune\relax }}{42}%
|
||||||
\contentsline {figure}{\numberline {2.8}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{46}%
|
\contentsline {figure}{\numberline {2.8}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{42}%
|
||||||
\contentsline {figure}{\numberline {2.9}{\ignorespaces Chute de la Lune sur la Terre\relax }}{46}%
|
\contentsline {figure}{\numberline {2.9}{\ignorespaces Chute de la Lune sur la Terre\relax }}{42}%
|
||||||
\contentsline {figure}{\numberline {2.10}{\ignorespaces Mouvement circulaire uniforme\relax }}{48}%
|
\contentsline {figure}{\numberline {2.10}{\ignorespaces Mouvement circulaire uniforme\relax }}{44}%
|
||||||
\contentsline {figure}{\numberline {2.11}{\ignorespaces Astronomica pars Optica}}{49}%
|
\contentsline {figure}{\numberline {2.11}{\ignorespaces Astronomica pars Optica}}{45}%
|
||||||
\contentsline {figure}{\numberline {2.12}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de cin\IeC {\'e}matique\relax }}{50}%
|
\contentsline {figure}{\numberline {2.12}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de cin\IeC {\'e}matique\relax }}{46}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {3.1}{\ignorespaces La balance de Cavendish}}{58}%
|
\contentsline {figure}{\numberline {3.1}{\ignorespaces La balance de Cavendish}}{54}%
|
||||||
\contentsline {figure}{\numberline {3.2}{\ignorespaces Loi de la gravitation universelle.\relax }}{59}%
|
\contentsline {figure}{\numberline {3.2}{\ignorespaces Loi de la gravitation universelle.\relax }}{55}%
|
||||||
\contentsline {figure}{\numberline {3.3}{\ignorespaces Poids apparent\relax }}{61}%
|
\contentsline {figure}{\numberline {3.3}{\ignorespaces Poids apparent\relax }}{57}%
|
||||||
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {a<0}}}{61}%
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {a<0}}}{57}%
|
||||||
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {a=0}}}{61}%
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {a=0}}}{57}%
|
||||||
\contentsline {subfigure}{\numberline {(c)}{\ignorespaces {a>0}}}{61}%
|
\contentsline {subfigure}{\numberline {(c)}{\ignorespaces {a>0}}}{57}%
|
||||||
\contentsline {figure}{\numberline {3.4}{\ignorespaces La sensation des mouvements}}{62}%
|
\contentsline {figure}{\numberline {3.4}{\ignorespaces La sensation des mouvements}}{58}%
|
||||||
\contentsline {figure}{\numberline {3.5}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{63}%
|
\contentsline {figure}{\numberline {3.5}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{59}%
|
||||||
\contentsline {figure}{\numberline {3.6}{\ignorespaces Pleines et basses mers\relax }}{65}%
|
\contentsline {figure}{\numberline {3.6}{\ignorespaces Pleines et basses mers\relax }}{61}%
|
||||||
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Logique mais faux}}}{65}%
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Logique mais faux}}}{61}%
|
||||||
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Le cas r\IeC {\'e}el}}}{65}%
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Le cas r\IeC {\'e}el}}}{61}%
|
||||||
\contentsline {figure}{\numberline {3.7}{\ignorespaces Syst\IeC {\`e}me Terre-Lune}}{67}%
|
\contentsline {figure}{\numberline {3.7}{\ignorespaces Syst\IeC {\`e}me Terre-Lune}}{63}%
|
||||||
\contentsline {figure}{\numberline {3.8}{\ignorespaces Construction de Proctor}}{67}%
|
\contentsline {figure}{\numberline {3.8}{\ignorespaces Construction de Proctor}}{63}%
|
||||||
\contentsline {figure}{\numberline {3.9}{\ignorespaces Force de mar\IeC {\'e}e}}{68}%
|
\contentsline {figure}{\numberline {3.9}{\ignorespaces Force de mar\IeC {\'e}e}}{64}%
|
||||||
\contentsline {figure}{\numberline {3.10}{\ignorespaces La force de frottement\relax }}{69}%
|
\contentsline {figure}{\numberline {3.10}{\ignorespaces La force de frottement\relax }}{65}%
|
||||||
\contentsline {figure}{\numberline {3.11}{\ignorespaces Freins de wagon\relax }}{70}%
|
\contentsline {figure}{\numberline {3.11}{\ignorespaces Freins de wagon\relax }}{66}%
|
||||||
\contentsline {figure}{\numberline {3.12}{\ignorespaces Essieu de wagon\relax }}{70}%
|
\contentsline {figure}{\numberline {3.12}{\ignorespaces Essieu de wagon\relax }}{66}%
|
||||||
\contentsline {figure}{\numberline {3.13}{\ignorespaces Force \IeC {\'e}lastique d'un ressort\relax }}{70}%
|
\contentsline {figure}{\numberline {3.13}{\ignorespaces Force \IeC {\'e}lastique d'un ressort\relax }}{66}%
|
||||||
\contentsline {figure}{\numberline {3.14}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de m\IeC {\'e}canique\relax }}{72}%
|
\contentsline {figure}{\numberline {3.14}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de m\IeC {\'e}canique\relax }}{68}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {4.1}{\ignorespaces Puissance}}{74}%
|
\contentsline {figure}{\numberline {4.1}{\ignorespaces \IeC {\'E}quilibre statique\relax }}{71}%
|
||||||
\contentsline {figure}{\numberline {4.2}{\ignorespaces \IeC {\'E}nergie cin\IeC {\'e}tique et potentielle}}{76}%
|
\contentsline {figure}{\numberline {4.2}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{72}%
|
||||||
\contentsline {figure}{\numberline {4.3}{\ignorespaces Barrage d'Emosson}}{78}%
|
\contentsline {figure}{\numberline {4.3}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{73}%
|
||||||
\contentsline {figure}{\numberline {4.4}{\ignorespaces Turbine Pelton}}{79}%
|
\contentsline {figure}{\numberline {4.4}{\ignorespaces Tir balistique\relax }}{74}%
|
||||||
\contentsline {figure}{\numberline {4.5}{\ignorespaces Ancienne turbine Pelton}}{79}%
|
\contentsline {figure}{\numberline {4.5}{\ignorespaces Tirs balistiques\relax }}{76}%
|
||||||
\contentsline {figure}{\numberline {4.6}{\ignorespaces \IeC {\'E}olienne}}{80}%
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Deux angles}}}{76}%
|
||||||
\contentsline {figure}{\numberline {4.7}{\ignorespaces Pale d'\IeC {\'e}olienne}}{80}%
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Un angle}}}{76}%
|
||||||
\contentsline {figure}{\numberline {4.8}{\ignorespaces Tube de vent\relax }}{81}%
|
\contentsline {figure}{\numberline {4.6}{\ignorespaces Parabole de s\IeC {\'e}curit\IeC {\'e}\relax }}{76}%
|
||||||
\contentsline {figure}{\numberline {4.9}{\ignorespaces Solaire thermique}}{83}%
|
\contentsline {figure}{\numberline {4.7}{\ignorespaces Mouvement circulaire uniforme\relax }}{77}%
|
||||||
\contentsline {figure}{\numberline {4.10}{\ignorespaces Effet photo\IeC {\'e}lectrique}}{83}%
|
\contentsline {figure}{\numberline {4.8}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse minimale\relax }}{78}%
|
||||||
\contentsline {figure}{\numberline {4.11}{\ignorespaces Cellule photo\IeC {\'e}lectrique}}{84}%
|
\contentsline {figure}{\numberline {4.9}{\ignorespaces Virages inclin\IeC {\'e}~: vitesses minimale\relax }}{78}%
|
||||||
\contentsline {figure}{\numberline {4.12}{\ignorespaces Applications de la g\IeC {\'e}othermie}}{85}%
|
\contentsline {figure}{\numberline {4.10}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse maximale\relax }}{79}%
|
||||||
\contentsline {figure}{\numberline {4.13}{\ignorespaces Fission de l'uranium\relax }}{86}%
|
|
||||||
\contentsline {figure}{\numberline {4.14}{\ignorespaces R\IeC {\'e}acteur nucl\IeC {\'e}aire\relax }}{86}%
|
|
||||||
\contentsline {figure}{\numberline {4.15}{\ignorespaces Combustion du m\IeC {\'e}thane}}{88}%
|
|
||||||
\contentsline {figure}{\numberline {4.16}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de l'\IeC {\'e}nergie\relax }}{89}%
|
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {5.1}{\ignorespaces Thermom\IeC {\`e}tres}}{92}%
|
\contentsline {figure}{\numberline {5.1}{\ignorespaces Chute visqueuse\relax }}{86}%
|
||||||
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Fahrenheit}}}{92}%
|
\contentsline {figure}{\numberline {5.2}{\ignorespaces Chute dans un fluide visqueux\relax }}{87}%
|
||||||
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Kelvin}}}{92}%
|
\contentsline {figure}{\numberline {5.3}{\ignorespaces Masse oscillante\relax }}{87}%
|
||||||
\contentsline {figure}{\numberline {5.2}{\ignorespaces Changements d'\IeC {\'e}tats\relax }}{94}%
|
\contentsline {figure}{\numberline {5.4}{\ignorespaces Masse suspendue\relax }}{88}%
|
||||||
\contentsline {figure}{\numberline {5.3}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de thermodynamique\relax }}{96}%
|
\contentsline {figure}{\numberline {5.5}{\ignorespaces Masse oscillante suspendue\relax }}{89}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {A.1}{\ignorespaces Relation de l'arc de cercle\relax }}{99}%
|
\contentsline {figure}{\numberline {6.1}{\ignorespaces Choc 2 dim}}{95}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {B.1}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires\relax }}{103}%
|
\contentsline {figure}{\numberline {7.1}{\ignorespaces Puissance}}{98}%
|
||||||
\contentsline {figure}{\numberline {B.2}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es sph\IeC {\'e}riques\relax }}{104}%
|
\contentsline {figure}{\numberline {7.2}{\ignorespaces \IeC {\'E}nergie cin\IeC {\'e}tique et potentielle}}{100}%
|
||||||
|
\contentsline {figure}{\numberline {7.3}{\ignorespaces Barrage d'Emosson}}{102}%
|
||||||
|
\contentsline {figure}{\numberline {7.4}{\ignorespaces Turbine Pelton}}{103}%
|
||||||
|
\contentsline {figure}{\numberline {7.5}{\ignorespaces Ancienne turbine Pelton}}{103}%
|
||||||
|
\contentsline {figure}{\numberline {7.6}{\ignorespaces \IeC {\'E}olienne}}{104}%
|
||||||
|
\contentsline {figure}{\numberline {7.7}{\ignorespaces Pale d'\IeC {\'e}olienne}}{104}%
|
||||||
|
\contentsline {figure}{\numberline {7.8}{\ignorespaces Tube de vent\relax }}{105}%
|
||||||
|
\contentsline {figure}{\numberline {7.9}{\ignorespaces Solaire thermique}}{107}%
|
||||||
|
\contentsline {figure}{\numberline {7.10}{\ignorespaces Effet photo\IeC {\'e}lectrique}}{107}%
|
||||||
|
\contentsline {figure}{\numberline {7.11}{\ignorespaces Cellule photo\IeC {\'e}lectrique}}{108}%
|
||||||
|
\contentsline {figure}{\numberline {7.12}{\ignorespaces Applications de la g\IeC {\'e}othermie}}{109}%
|
||||||
|
\contentsline {figure}{\numberline {7.13}{\ignorespaces Fission de l'uranium\relax }}{110}%
|
||||||
|
\contentsline {figure}{\numberline {7.14}{\ignorespaces R\IeC {\'e}acteur nucl\IeC {\'e}aire\relax }}{110}%
|
||||||
|
\contentsline {figure}{\numberline {7.15}{\ignorespaces Combustion du m\IeC {\'e}thane}}{112}%
|
||||||
|
\contentsline {figure}{\numberline {7.16}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de l'\IeC {\'e}nergie\relax }}{113}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {C.1}{\ignorespaces Taille de la terre\relax }}{105}%
|
\contentsline {figure}{\numberline {8.1}{\ignorespaces \IeC {\'E}nergie et vitesse\relax }}{115}%
|
||||||
\contentsline {figure}{\numberline {C.2}{\ignorespaces Taille de la lune}}{107}%
|
\contentsline {figure}{\numberline {8.2}{\ignorespaces Balance \IeC {\`a} fl\IeC {\'e}au\relax }}{115}%
|
||||||
\contentsline {figure}{\numberline {C.3}{\ignorespaces Parallaxe de Mars}}{108}%
|
\contentsline {figure}{\numberline {8.3}{\ignorespaces Travail simple\relax }}{116}%
|
||||||
|
\contentsline {figure}{\numberline {8.4}{\ignorespaces Travail et produit scalaire\relax }}{116}%
|
||||||
|
\contentsline {figure}{\numberline {8.5}{\ignorespaces Travail en g\IeC {\'e}n\IeC {\'e}ral\relax }}{116}%
|
||||||
|
\contentsline {figure}{\numberline {8.6}{\ignorespaces Travail du poids\relax }}{121}%
|
||||||
|
\contentsline {figure}{\numberline {8.7}{\ignorespaces Force et \IeC {\'e}nergie potentielle de gravitation entre la Terre et le Soleil\relax }}{123}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {D.1}{\ignorespaces Rail horizontal}}{112}%
|
|
||||||
\contentsline {figure}{\numberline {D.2}{\ignorespaces Chute libre\relax }}{113}%
|
|
||||||
\contentsline {figure}{\numberline {D.3}{\ignorespaces Une pendule\relax }}{116}%
|
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {E.1}{\ignorespaces Le syst\IeC {\`e}me g\IeC {\'e}ocentrique de Tycho Brah\IeC {\'e}}}{122}%
|
\contentsline {figure}{\numberline {10.1}{\ignorespaces Thermom\IeC {\`e}tres}}{130}%
|
||||||
\contentsline {figure}{\numberline {E.2}{\ignorespaces Le Soleil dans la Voie Lact\IeC {\'e}e}}{123}%
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Fahrenheit}}}{130}%
|
||||||
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Kelvin}}}{130}%
|
||||||
|
\contentsline {figure}{\numberline {10.2}{\ignorespaces Changements d'\IeC {\'e}tats\relax }}{132}%
|
||||||
|
\contentsline {figure}{\numberline {10.3}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de thermodynamique\relax }}{134}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {F.1}{\ignorespaces \emph {Discours concernant deux sciences nouvelles} de Galil\IeC {\'e}e}}{125}%
|
\contentsline {figure}{\numberline {11.1}{\ignorespaces Dilatation lin\IeC {\'e}aire\relax }}{136}%
|
||||||
|
\contentsline {figure}{\numberline {11.2}{\ignorespaces Fusible bilame\relax }}{136}%
|
||||||
|
\contentsline {figure}{\numberline {11.3}{\ignorespaces Dilatation volumique\relax }}{137}%
|
||||||
|
\contentsline {figure}{\numberline {11.4}{\ignorespaces Travail et diagramme P-V\relax }}{144}%
|
||||||
|
\contentsline {figure}{\numberline {11.5}{\ignorespaces Transformation isobare\relax }}{146}%
|
||||||
|
\contentsline {figure}{\numberline {11.6}{\ignorespaces Transformation isochore\relax }}{147}%
|
||||||
|
\contentsline {figure}{\numberline {11.7}{\ignorespaces Transformation isotherme\relax }}{147}%
|
||||||
|
\contentsline {figure}{\numberline {11.8}{\ignorespaces Transformation adiabatique\relax }}{148}%
|
||||||
|
\contentsline {figure}{\numberline {11.9}{\ignorespaces Moteur thermique}}{151}%
|
||||||
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Chargement}}}{151}%
|
||||||
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Chauffage}}}{151}%
|
||||||
|
\contentsline {subfigure}{\numberline {(c)}{\ignorespaces {D\IeC {\'e}chargement}}}{151}%
|
||||||
|
\contentsline {subfigure}{\numberline {(d)}{\ignorespaces {Refroidissement}}}{151}%
|
||||||
|
\contentsline {figure}{\numberline {11.10}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{151}%
|
||||||
|
\contentsline {figure}{\numberline {11.11}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{152}%
|
||||||
|
\contentsline {figure}{\numberline {11.12}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{152}%
|
||||||
|
\contentsline {figure}{\numberline {11.13}{\ignorespaces Moteur \IeC {\`a} explosion}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(a)}{\ignorespaces {Admission}}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(b)}{\ignorespaces {Compression}}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(c)}{\ignorespaces {Allumage}}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(d)}{\ignorespaces {Temps moteur}}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(e)}{\ignorespaces {\IeC {\'E}chappement}}}{153}%
|
||||||
|
\contentsline {subfigure}{\numberline {(f)}{\ignorespaces {\IeC {\'E}vacuation}}}{153}%
|
||||||
|
\contentsline {figure}{\numberline {11.14}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{153}%
|
||||||
|
\contentsline {figure}{\numberline {11.15}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{154}%
|
||||||
|
\contentsline {figure}{\numberline {11.16}{\ignorespaces Le cycle de Carnot\relax }}{156}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {G.1}{\ignorespaces Chute de la lune\relax }}{127}%
|
\contentsline {figure}{\numberline {A.1}{\ignorespaces Relation de l'arc de cercle\relax }}{161}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {H.1}{\ignorespaces Satellite}}{129}%
|
\contentsline {figure}{\numberline {B.1}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires\relax }}{165}%
|
||||||
|
\contentsline {figure}{\numberline {B.2}{\ignorespaces Syst\IeC {\`e}me de coordonn\IeC {\'e}es sph\IeC {\'e}riques\relax }}{166}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {I.1}{\ignorespaces Transformation de galil\IeC {\'e}e}}{132}%
|
\contentsline {figure}{\numberline {C.1}{\ignorespaces Taille de la terre\relax }}{167}%
|
||||||
\contentsline {figure}{\numberline {J.1}{\ignorespaces Mar\IeC {\'e}e}}{135}%
|
\contentsline {figure}{\numberline {C.2}{\ignorespaces Taille de la lune}}{169}%
|
||||||
|
\contentsline {figure}{\numberline {C.3}{\ignorespaces Parallaxe de Mars}}{170}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {J.2}{\ignorespaces Syst\IeC {\`e}me Terre-Lune\relax }}{136}%
|
\contentsline {figure}{\numberline {D.1}{\ignorespaces Rail horizontal}}{174}%
|
||||||
\contentsline {figure}{\numberline {J.3}{\ignorespaces Syst\IeC {\`e}me Terre-Lune-eau\relax }}{136}%
|
\contentsline {figure}{\numberline {D.2}{\ignorespaces Chute libre\relax }}{175}%
|
||||||
\contentsline {figure}{\numberline {J.4}{\ignorespaces D\IeC {\'e}calage horaire}}{138}%
|
\contentsline {figure}{\numberline {D.3}{\ignorespaces Une pendule\relax }}{178}%
|
||||||
\contentsline {figure}{\numberline {J.5}{\ignorespaces Vives et mortes eaux}}{138}%
|
|
||||||
\contentsline {figure}{\numberline {J.6}{\ignorespaces Limite de Roche}}{140}%
|
|
||||||
\contentsline {figure}{\numberline {J.7}{\ignorespaces Limite de Roche}}{141}%
|
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {K.1}{\ignorespaces Le barrage du Ch\IeC {\^a}telot}}{143}%
|
\contentsline {figure}{\numberline {E.1}{\ignorespaces Le syst\IeC {\`e}me g\IeC {\'e}ocentrique de Tycho Brah\IeC {\'e}}}{184}%
|
||||||
|
\contentsline {figure}{\numberline {E.2}{\ignorespaces Le Soleil dans la Voie Lact\IeC {\'e}e}}{185}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {L.1}{\ignorespaces Le rayon de la Terre par Eratosth\IeC {\`e}ne\relax }}{148}%
|
\contentsline {figure}{\numberline {F.1}{\ignorespaces \emph {Discours concernant deux sciences nouvelles} de Galil\IeC {\'e}e}}{187}%
|
||||||
\contentsline {figure}{\numberline {L.2}{\ignorespaces La poulie}}{151}%
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {L.3}{\ignorespaces Graphes horaires du MRU.\relax }}{157}%
|
\contentsline {figure}{\numberline {G.1}{\ignorespaces Chute de la lune\relax }}{189}%
|
||||||
\contentsline {figure}{\numberline {L.4}{\ignorespaces Chute aristot\IeC {\'e}licienne de la tour Eiffel.\relax }}{160}%
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {L.5}{\ignorespaces Une fus\IeC {\'e}e.\relax }}{160}%
|
\contentsline {figure}{\numberline {H.1}{\ignorespaces Satellite}}{191}%
|
||||||
\contentsline {figure}{\numberline {L.6}{\ignorespaces Une remorque\relax }}{161}%
|
\addvspace {10\p@ }
|
||||||
\contentsline {figure}{\numberline {L.7}{\ignorespaces Un ascenseur\relax }}{164}%
|
\contentsline {figure}{\numberline {I.1}{\ignorespaces Transformation de galil\IeC {\'e}e}}{194}%
|
||||||
|
\contentsline {figure}{\numberline {J.1}{\ignorespaces Mar\IeC {\'e}e}}{197}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {figure}{\numberline {J.2}{\ignorespaces Syst\IeC {\`e}me Terre-Lune\relax }}{198}%
|
||||||
|
\contentsline {figure}{\numberline {J.3}{\ignorespaces Syst\IeC {\`e}me Terre-Lune-eau\relax }}{198}%
|
||||||
|
\contentsline {figure}{\numberline {J.4}{\ignorespaces D\IeC {\'e}calage horaire}}{200}%
|
||||||
|
\contentsline {figure}{\numberline {J.5}{\ignorespaces Vives et mortes eaux}}{200}%
|
||||||
|
\contentsline {figure}{\numberline {J.6}{\ignorespaces Limite de Roche}}{202}%
|
||||||
|
\contentsline {figure}{\numberline {J.7}{\ignorespaces Limite de Roche}}{203}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {figure}{\numberline {K.1}{\ignorespaces Le barrage du Ch\IeC {\^a}telot}}{205}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {figure}{\numberline {L.1}{\ignorespaces Le rayon de la Terre par Eratosth\IeC {\`e}ne\relax }}{210}%
|
||||||
|
\contentsline {figure}{\numberline {L.2}{\ignorespaces La poulie}}{213}%
|
||||||
|
\contentsline {figure}{\numberline {L.3}{\ignorespaces Masse pendante}}{214}%
|
||||||
|
\contentsline {figure}{\numberline {L.4}{\ignorespaces Deux poulies}}{214}%
|
||||||
|
\contentsline {figure}{\numberline {L.5}{\ignorespaces Bloc suspendu}}{216}%
|
||||||
|
\contentsline {figure}{\numberline {L.6}{\ignorespaces Graphes horaires du MRU.\relax }}{221}%
|
||||||
|
\contentsline {figure}{\numberline {L.7}{\ignorespaces Chute aristot\IeC {\'e}licienne de la tour Eiffel.\relax }}{224}%
|
||||||
|
\contentsline {figure}{\numberline {L.8}{\ignorespaces Une fus\IeC {\'e}e.\relax }}{224}%
|
||||||
|
\contentsline {figure}{\numberline {L.9}{\ignorespaces Une remorque\relax }}{225}%
|
||||||
|
\contentsline {figure}{\numberline {L.10}{\ignorespaces Un ascenseur\relax }}{228}%
|
||||||
|
\contentsline {figure}{\numberline {L.11}{\ignorespaces Force inclin\IeC {\'e}e}}{233}%
|
||||||
|
\contentsline {figure}{\numberline {L.12}{\ignorespaces Lampe suspendue}}{234}%
|
||||||
|
\contentsline {figure}{\numberline {L.13}{\ignorespaces Plan inclin\IeC {\'e}}}{235}%
|
||||||
|
\contentsline {figure}{\numberline {L.14}{\ignorespaces Corde poulie}}{238}%
|
||||||
|
\contentsline {figure}{\numberline {L.15}{\ignorespaces Corde tir\IeC {\'e}e poulie}}{238}%
|
||||||
|
\contentsline {figure}{\numberline {L.16}{\ignorespaces Corde tir\IeC {\'e}e poulie juste}}{238}%
|
||||||
|
\contentsline {figure}{\numberline {L.17}{\ignorespaces Frottements}}{241}%
|
||||||
|
\contentsline {figure}{\numberline {L.18}{\ignorespaces Forces sur bloc suspendu}}{242}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {figure}{\numberline {M.1}{\ignorespaces Baguettes d'une ann\IeC {\'e}e\relax }}{248}%
|
||||||
|
|||||||
File diff suppressed because it is too large
Load Diff
@ -1,25 +1,10 @@
|
|||||||
\babel@toc {french}{}
|
\babel@toc {french}{}
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {table}{\numberline {1.1}{\ignorespaces Tableau des particules \IeC {\'e}l\IeC {\'e}mentaires}}{34}%
|
\contentsline {table}{\numberline {1.1}{\ignorespaces Tableau des particules \IeC {\'e}l\IeC {\'e}mentaires}}{30}%
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\contentsline {table}{\numberline {2.1}{\ignorespaces Donn\IeC {\'e}es de la mission Apollo 12\relax }}{40}%
|
\contentsline {table}{\numberline {2.1}{\ignorespaces Donn\IeC {\'e}es de la mission Apollo 12\relax }}{36}%
|
||||||
\contentsline {table}{\numberline {2.2}{\ignorespaces La hauteur en fonction du temps\relax }}{42}%
|
\contentsline {table}{\numberline {2.2}{\ignorespaces La hauteur en fonction du temps\relax }}{38}%
|
||||||
\contentsline {table}{\numberline {2.3}{\ignorespaces La vitesse en fonction du temps\relax }}{43}%
|
\contentsline {table}{\numberline {2.3}{\ignorespaces La vitesse en fonction du temps\relax }}{39}%
|
||||||
\addvspace {10\p@ }
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\contentsline {table}{\numberline {5.1}{\ignorespaces C\oe fficient de dilatation lin\IeC {\'e}aire\relax }}{93}%
|
|
||||||
\contentsline {table}{\numberline {5.2}{\ignorespaces Chaleur sp\IeC {\'e}cifique\relax }}{93}%
|
|
||||||
\contentsline {table}{\numberline {5.3}{\ignorespaces Chaleur latente\relax }}{94}%
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\contentsline {table}{\numberline {A.1}{\ignorespaces Les unit\IeC {\'e}s du Syst\IeC {\`e}me International\relax }}{100}%
|
|
||||||
\contentsline {table}{\numberline {A.2}{\ignorespaces Conversions d'unit\IeC {\'e}s\relax }}{100}%
|
|
||||||
\contentsline {table}{\numberline {A.3}{\ignorespaces Quelques \IeC {\'e}quivalents\relax }}{100}%
|
|
||||||
\contentsline {table}{\numberline {A.4}{\ignorespaces Multiples et sous-multiples\relax }}{101}%
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\addvspace {10\p@ }
|
|
||||||
\contentsline {table}{\numberline {D.1}{\ignorespaces Tableau de mesures\relax }}{113}%
|
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
@ -28,3 +13,34 @@
|
|||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
\addvspace {10\p@ }
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {table}{\numberline {10.1}{\ignorespaces C\oe fficient de dilatation lin\IeC {\'e}aire\relax }}{131}%
|
||||||
|
\contentsline {table}{\numberline {10.2}{\ignorespaces Chaleur sp\IeC {\'e}cifique\relax }}{131}%
|
||||||
|
\contentsline {table}{\numberline {10.3}{\ignorespaces Chaleur latente\relax }}{132}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {table}{\numberline {11.1}{\ignorespaces Coefficient de dilatation lin\IeC {\'e}aire\relax }}{136}%
|
||||||
|
\contentsline {table}{\numberline {11.2}{\ignorespaces Coefficient de dilatation volumique\relax }}{137}%
|
||||||
|
\contentsline {table}{\numberline {11.3}{\ignorespaces Chaleur massique\relax }}{138}%
|
||||||
|
\contentsline {table}{\numberline {11.4}{\ignorespaces Chaleur latente\relax }}{139}%
|
||||||
|
\contentsline {table}{\numberline {11.5}{\ignorespaces \IeC {\'E}tats caract\IeC {\'e}ristiques\relax }}{150}%
|
||||||
|
\contentsline {table}{\numberline {11.6}{\ignorespaces Grandeurs caract\IeC {\'e}ristiques\relax }}{152}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {table}{\numberline {A.1}{\ignorespaces Les unit\IeC {\'e}s du Syst\IeC {\`e}me International\relax }}{162}%
|
||||||
|
\contentsline {table}{\numberline {A.2}{\ignorespaces Conversions d'unit\IeC {\'e}s\relax }}{162}%
|
||||||
|
\contentsline {table}{\numberline {A.3}{\ignorespaces Quelques \IeC {\'e}quivalents\relax }}{162}%
|
||||||
|
\contentsline {table}{\numberline {A.4}{\ignorespaces Multiples et sous-multiples\relax }}{163}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {table}{\numberline {D.1}{\ignorespaces Tableau de mesures\relax }}{175}%
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\addvspace {10\p@ }
|
||||||
|
\contentsline {table}{\numberline {M.1}{\ignorespaces La longueur des baguettes de pain\relax }}{246}%
|
||||||
|
\contentsline {table}{\numberline {M.2}{\ignorespaces La longueur d'autres baguettes de pain\relax }}{247}%
|
||||||
|
\contentsline {table}{\numberline {M.3}{\ignorespaces Des centaines de baguettes de pain\relax }}{247}%
|
||||||
|
|||||||
Binary file not shown.
98463
CoursMecaniqueOSDF.ps
98463
CoursMecaniqueOSDF.ps
File diff suppressed because it is too large
Load Diff
@ -8,8 +8,8 @@
|
|||||||
\usepackage[arrow,matrix,tips,frame]{xy}
|
\usepackage[arrow,matrix,tips,frame]{xy}
|
||||||
%\renewcommand{\bibname}{Bibliographie}
|
%\renewcommand{\bibname}{Bibliographie}
|
||||||
|
|
||||||
\usepackage[DF]{optional} % Pour réaliser le cours de base de Discipline Fondamentale (DF)
|
%\usepackage[DF]{optional} % Pour réaliser le cours de base de Discipline Fondamentale (DF)
|
||||||
%\usepackage[OS]{optional} % Pour réaliser le cours complet d'Option Spécifique (OS)
|
\usepackage[OS]{optional} % Pour réaliser le cours complet d'Option Spécifique (OS)
|
||||||
% La commande pour ajouter les parties d'OS est \opt{OS}{parties}
|
% La commande pour ajouter les parties d'OS est \opt{OS}{parties}
|
||||||
|
|
||||||
%---------------------------------------------------------------
|
%---------------------------------------------------------------
|
||||||
|
|||||||
@ -1,262 +1,421 @@
|
|||||||
\babel@toc {french}{}
|
\babel@toc {french}{}
|
||||||
\contentsline {chapter}{\numberline {1}Introduction}{21}%
|
\contentsline {chapter}{\numberline {1}Introduction}{17}%
|
||||||
\contentsline {section}{\numberline {1.1}Du temps}{21}%
|
\contentsline {section}{\numberline {1.1}Du temps}{17}%
|
||||||
\contentsline {section}{\numberline {1.2}De l'infiniment grand \IeC {\`a} l'infiniment petit}{21}%
|
\contentsline {section}{\numberline {1.2}De l'infiniment grand \IeC {\`a} l'infiniment petit}{17}%
|
||||||
\contentsline {subsection}{\numberline {1.2.1}L'Univers}{21}%
|
\contentsline {subsection}{\numberline {1.2.1}L'Univers}{17}%
|
||||||
\contentsline {subsection}{\numberline {1.2.2}Les amas de galaxies}{22}%
|
\contentsline {subsection}{\numberline {1.2.2}Les amas de galaxies}{18}%
|
||||||
\contentsline {subsection}{\numberline {1.2.3}Les galaxies}{23}%
|
\contentsline {subsection}{\numberline {1.2.3}Les galaxies}{19}%
|
||||||
\contentsline {subsection}{\numberline {1.2.4}Les \IeC {\'e}toiles}{24}%
|
\contentsline {subsection}{\numberline {1.2.4}Les \IeC {\'e}toiles}{20}%
|
||||||
\contentsline {subsection}{\numberline {1.2.5}Le syst\IeC {\`e}me solaire}{24}%
|
\contentsline {subsection}{\numberline {1.2.5}Le syst\IeC {\`e}me solaire}{20}%
|
||||||
\contentsline {subsection}{\numberline {1.2.6}La Terre et la Lune}{26}%
|
\contentsline {subsection}{\numberline {1.2.6}La Terre et la Lune}{22}%
|
||||||
\contentsline {subsubsection}{La Terre}{26}%
|
\contentsline {subsubsection}{La Terre}{22}%
|
||||||
\contentsline {subsubsection}{La Lune}{27}%
|
\contentsline {subsubsection}{La Lune}{23}%
|
||||||
\contentsline {subsubsection}{Les mar\IeC {\'e}es}{29}%
|
\contentsline {subsubsection}{Les mar\IeC {\'e}es}{25}%
|
||||||
\contentsline {subsection}{\numberline {1.2.7}Le monde subatomique}{32}%
|
\contentsline {subsection}{\numberline {1.2.7}Le monde subatomique}{28}%
|
||||||
\contentsline {subsubsection}{Conclusion}{36}%
|
\contentsline {subsubsection}{Conclusion}{32}%
|
||||||
\contentsline {chapter}{\numberline {2}La cin\IeC {\'e}matique}{37}%
|
\contentsline {chapter}{\numberline {2}La cin\IeC {\'e}matique}{33}%
|
||||||
\contentsline {section}{\numberline {2.1}Introduction}{37}%
|
\contentsline {section}{\numberline {2.1}Introduction}{33}%
|
||||||
\contentsline {section}{\numberline {2.2}Position}{37}%
|
\contentsline {section}{\numberline {2.2}Position}{33}%
|
||||||
\contentsline {subsection}{\numberline {2.2.1}Dimensions}{37}%
|
\contentsline {subsection}{\numberline {2.2.1}Dimensions}{33}%
|
||||||
\contentsline {subsection}{\numberline {2.2.2}Syst\IeC {\`e}me d'axes}{37}%
|
\contentsline {subsection}{\numberline {2.2.2}Syst\IeC {\`e}me d'axes}{33}%
|
||||||
\contentsline {subsection}{\numberline {2.2.3}Position}{37}%
|
\contentsline {subsection}{\numberline {2.2.3}Position}{33}%
|
||||||
\contentsline {subsection}{\numberline {2.2.4}D\IeC {\'e}placement}{38}%
|
\contentsline {subsection}{\numberline {2.2.4}D\IeC {\'e}placement}{34}%
|
||||||
\contentsline {subsection}{\numberline {2.2.5}Distance parcourue}{38}%
|
\contentsline {subsection}{\numberline {2.2.5}Distance parcourue}{34}%
|
||||||
\contentsline {section}{\numberline {2.3}Vitesse}{38}%
|
\contentsline {section}{\numberline {2.3}Vitesse}{34}%
|
||||||
\contentsline {subsection}{\numberline {2.3.1}Vitesse moyenne}{38}%
|
\contentsline {subsection}{\numberline {2.3.1}Vitesse moyenne}{34}%
|
||||||
\contentsline {subsection}{\numberline {2.3.2}Exemples}{38}%
|
\contentsline {subsection}{\numberline {2.3.2}Exemples}{34}%
|
||||||
\contentsline {subsubsection}{Exemple 1}{38}%
|
\contentsline {subsubsection}{Exemple 1}{34}%
|
||||||
\contentsline {subsubsection}{Exemple 2}{38}%
|
\contentsline {subsubsection}{Exemple 2}{34}%
|
||||||
\contentsline {subsection}{\numberline {2.3.3}Vitesse instantan\IeC {\'e}e}{38}%
|
\contentsline {subsection}{\numberline {2.3.3}Vitesse instantan\IeC {\'e}e}{34}%
|
||||||
\contentsline {section}{\numberline {2.4}Acc\IeC {\'e}l\IeC {\'e}ration}{39}%
|
\contentsline {section}{\numberline {2.4}Acc\IeC {\'e}l\IeC {\'e}ration}{35}%
|
||||||
\contentsline {subsection}{\numberline {2.4.1}Acc\IeC {\'e}l\IeC {\'e}ration moyenne}{39}%
|
\contentsline {subsection}{\numberline {2.4.1}Acc\IeC {\'e}l\IeC {\'e}ration moyenne}{35}%
|
||||||
\contentsline {subsection}{\numberline {2.4.2}Exemples}{39}%
|
\contentsline {subsection}{\numberline {2.4.2}Exemples}{35}%
|
||||||
\contentsline {subsubsection}{Exemple 1}{39}%
|
\contentsline {subsubsection}{Exemple 1}{35}%
|
||||||
\contentsline {subsubsection}{Exemple 2}{39}%
|
\contentsline {subsubsection}{Exemple 2}{35}%
|
||||||
\contentsline {subsubsection}{Remarque~:}{39}%
|
\contentsline {subsubsection}{Remarque~:}{35}%
|
||||||
\contentsline {subsection}{\numberline {2.4.3}L'acc\IeC {\'e}l\IeC {\'e}ration instantan\IeC {\'e}e}{39}%
|
\contentsline {subsection}{\numberline {2.4.3}L'acc\IeC {\'e}l\IeC {\'e}ration instantan\IeC {\'e}e}{35}%
|
||||||
\contentsline {section}{\numberline {2.5}Mouvements simples}{39}%
|
\contentsline {section}{\numberline {2.5}Mouvements simples}{35}%
|
||||||
\contentsline {subsection}{\numberline {2.5.1}Le mouvement rectiligne uniforme}{39}%
|
\contentsline {subsection}{\numberline {2.5.1}Le mouvement rectiligne uniforme}{35}%
|
||||||
\contentsline {subsubsection}{D\IeC {\'e}finition}{39}%
|
\contentsline {subsubsection}{D\IeC {\'e}finition}{35}%
|
||||||
\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{39}%
|
\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{35}%
|
||||||
\contentsline {subsubsection}{Un exemple~: Apollo en route vers la Lune}{40}%
|
\contentsline {subsubsection}{Un exemple~: Apollo en route vers la Lune}{36}%
|
||||||
\contentsline {subsubsection}{Autre exemple~: le d\IeC {\'e}placement d'Androm\IeC {\`e}de}{41}%
|
\contentsline {subsubsection}{Autre exemple~: le d\IeC {\'e}placement d'Androm\IeC {\`e}de}{37}%
|
||||||
\contentsline {subsection}{\numberline {2.5.2}Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e} (MRUA)}{41}%
|
\contentsline {subsection}{\numberline {2.5.2}Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e} (MRUA)}{37}%
|
||||||
\contentsline {subsubsection}{D\IeC {\'e}finition}{41}%
|
\contentsline {subsubsection}{D\IeC {\'e}finition}{37}%
|
||||||
\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{41}%
|
\contentsline {subsubsection}{Propri\IeC {\'e}t\IeC {\'e}s}{37}%
|
||||||
\contentsline {subsection}{\numberline {2.5.3}La chute libre}{42}%
|
\contentsline {subsection}{\numberline {2.5.3}La chute libre}{38}%
|
||||||
\contentsline {paragraph}{D\IeC {\'e}finition}{42}%
|
\contentsline {paragraph}{D\IeC {\'e}finition}{38}%
|
||||||
\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{42}%
|
\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{38}%
|
||||||
\contentsline {paragraph}{Exp\IeC {\'e}rience}{42}%
|
\contentsline {paragraph}{Exp\IeC {\'e}rience}{38}%
|
||||||
\contentsline {paragraph}{Calculs}{42}%
|
\contentsline {paragraph}{Calculs}{38}%
|
||||||
\contentsline {paragraph}{Analyse des r\IeC {\'e}sultats}{43}%
|
\contentsline {paragraph}{Analyse des r\IeC {\'e}sultats}{39}%
|
||||||
\contentsline {paragraph}{Conclusions}{44}%
|
\contentsline {paragraph}{Conclusions}{40}%
|
||||||
\contentsline {subsection}{\numberline {2.5.4}Balistique}{44}%
|
\contentsline {subsection}{\numberline {2.5.4}Balistique}{40}%
|
||||||
\contentsline {paragraph}{D\IeC {\'e}finition}{44}%
|
\contentsline {paragraph}{D\IeC {\'e}finition}{40}%
|
||||||
\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{44}%
|
\contentsline {paragraph}{Propri\IeC {\'e}t\IeC {\'e}s}{40}%
|
||||||
\contentsline {paragraph}{\IeC {\'E}quations}{44}%
|
\contentsline {paragraph}{\IeC {\'E}quations}{40}%
|
||||||
\contentsline {paragraph}{Premier exemple}{45}%
|
\contentsline {paragraph}{Premier exemple}{41}%
|
||||||
\contentsline {paragraph}{Second exemple}{45}%
|
\contentsline {paragraph}{Second exemple}{41}%
|
||||||
\contentsline {subsection}{\numberline {2.5.5}La chute libre ... de la Lune}{45}%
|
\contentsline {subsection}{\numberline {2.5.5}La chute libre ... de la Lune}{41}%
|
||||||
\contentsline {subsection}{\numberline {2.5.6}Mouvement circulaire uniforme (MCU)}{47}%
|
\contentsline {subsection}{\numberline {2.5.6}Mouvement circulaire uniforme (MCU)}{43}%
|
||||||
\contentsline {subsubsection}{Relation importante}{47}%
|
\contentsline {subsubsection}{Relation importante}{43}%
|
||||||
\contentsline {subsection}{\numberline {2.5.7}Lois de Kepler}{48}%
|
\contentsline {subsection}{\numberline {2.5.7}Lois de Kepler}{44}%
|
||||||
\contentsline {chapter}{\numberline {3}La m\IeC {\'e}canique}{51}%
|
\contentsline {chapter}{\numberline {3}La m\IeC {\'e}canique}{47}%
|
||||||
\contentsline {section}{\numberline {3.1}La \FB@og m\IeC {\'e}canique\fg {} d'Aristote}{51}%
|
\contentsline {section}{\numberline {3.1}La \FB@og m\IeC {\'e}canique\fg {} d'Aristote}{47}%
|
||||||
\contentsline {subsection}{\numberline {3.1.1}Introduction}{51}%
|
\contentsline {subsection}{\numberline {3.1.1}Introduction}{47}%
|
||||||
\contentsline {subsection}{\numberline {3.1.2}Platon}{51}%
|
\contentsline {subsection}{\numberline {3.1.2}Platon}{47}%
|
||||||
\contentsline {subsection}{\numberline {3.1.3}Aristote}{52}%
|
\contentsline {subsection}{\numberline {3.1.3}Aristote}{48}%
|
||||||
\contentsline {subsubsection}{Cin\IeC {\'e}matique}{52}%
|
\contentsline {subsubsection}{Cin\IeC {\'e}matique}{48}%
|
||||||
\contentsline {subsubsection}{Dynamique}{52}%
|
\contentsline {subsubsection}{Dynamique}{48}%
|
||||||
\contentsline {section}{\numberline {3.2}M\IeC {\'e}canique de Newton}{55}%
|
\contentsline {section}{\numberline {3.2}M\IeC {\'e}canique de Newton}{51}%
|
||||||
\contentsline {subsection}{\numberline {3.2.1}Introduction}{55}%
|
\contentsline {subsection}{\numberline {3.2.1}Introduction}{51}%
|
||||||
\contentsline {subsection}{\numberline {3.2.2}M\IeC {\'e}canique}{55}%
|
\contentsline {subsection}{\numberline {3.2.2}M\IeC {\'e}canique}{51}%
|
||||||
\contentsline {subsubsection}{Les trois lois de Newton}{55}%
|
\contentsline {subsubsection}{Les trois lois de Newton}{51}%
|
||||||
\contentsline {subsubsection}{Force ext\IeC {\'e}rieure}{56}%
|
\contentsline {subsubsection}{Force ext\IeC {\'e}rieure}{52}%
|
||||||
\contentsline {subsubsection}{Exemples}{57}%
|
\contentsline {subsubsection}{Exemples}{53}%
|
||||||
\contentsline {subsection}{\numberline {3.2.3}Types de forces}{57}%
|
\contentsline {subsection}{\numberline {3.2.3}Types de forces}{53}%
|
||||||
\contentsline {subsubsection}{Loi de la gravitation universelle}{58}%
|
\contentsline {subsubsection}{Loi de la gravitation universelle}{54}%
|
||||||
\contentsline {subsubsection}{Le poids}{58}%
|
\contentsline {subsubsection}{Le poids}{54}%
|
||||||
\contentsline {paragraph}{Exemple}{59}%
|
\contentsline {paragraph}{Exemple}{55}%
|
||||||
\contentsline {subsubsection}{Masse et poids}{60}%
|
\contentsline {subsubsection}{Masse et poids}{56}%
|
||||||
\contentsline {subsubsection}{Poids apparent}{60}%
|
\contentsline {subsubsection}{Poids apparent}{56}%
|
||||||
\contentsline {subsubsection}{Gravitation et MCU}{62}%
|
\contentsline {subsubsection}{Gravitation et MCU}{58}%
|
||||||
\contentsline {subsubsection}{Troisi\IeC {\`e}me loi de Kepler}{63}%
|
\contentsline {subsubsection}{Troisi\IeC {\`e}me loi de Kepler}{59}%
|
||||||
\contentsline {subsubsection}{Les mar\IeC {\'e}es}{65}%
|
\contentsline {subsubsection}{Les mar\IeC {\'e}es}{61}%
|
||||||
\contentsline {subsubsection}{Le frottement}{69}%
|
\contentsline {subsubsection}{Le frottement}{65}%
|
||||||
\contentsline {paragraph}{Exemple}{70}%
|
\contentsline {paragraph}{Exemple}{66}%
|
||||||
\contentsline {subsubsection}{La force d'un ressort}{70}%
|
\contentsline {subsubsection}{La force d'un ressort}{66}%
|
||||||
\contentsline {paragraph}{Exemple}{70}%
|
\contentsline {paragraph}{Exemple}{66}%
|
||||||
\contentsline {chapter}{\numberline {4}L'\IeC {\'e}nergie}{73}%
|
\contentsline {chapter}{\numberline {4}M\IeC {\'e}canique en plusieurs dimensions}{69}%
|
||||||
\contentsline {section}{\numberline {4.1}Introduction}{73}%
|
\contentsline {section}{\numberline {4.1}Pr\IeC {\'e}liminaires}{69}%
|
||||||
\contentsline {section}{\numberline {4.2}Travail}{73}%
|
\contentsline {subsection}{\numberline {4.1.1}Dimensions}{69}%
|
||||||
\contentsline {section}{\numberline {4.3}Puissance}{74}%
|
\contentsline {subsection}{\numberline {4.1.2}Syst\IeC {\`e}me d'axes}{69}%
|
||||||
\contentsline {section}{\numberline {4.4}\IeC {\'E}nergie potentielle}{74}%
|
\contentsline {section}{\numberline {4.2}Notion de vecteur en physique}{69}%
|
||||||
\contentsline {section}{\numberline {4.5}\IeC {\'E}nergie cin\IeC {\'e}tique}{75}%
|
\contentsline {subsection}{\numberline {4.2.1}Norme d'un vecteur}{69}%
|
||||||
\contentsline {section}{\numberline {4.6}Th\IeC {\'e}or\IeC {\`e}me de l'\IeC {\'e}nergie cin\IeC {\'e}tique}{75}%
|
\contentsline {subsection}{\numberline {4.2.2}Op\IeC {\'e}rations vectorielles}{70}%
|
||||||
\contentsline {section}{\numberline {4.7}Conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{75}%
|
\contentsline {subsubsection}{produit scalaire}{70}%
|
||||||
\contentsline {section}{\numberline {4.8}Variation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{77}%
|
\contentsline {subsubsection}{Produit vectoriel}{70}%
|
||||||
\contentsline {section}{\numberline {4.9}\IeC {\'E}nergies renouvelables}{77}%
|
\contentsline {section}{\numberline {4.3}M\IeC {\'e}canique}{70}%
|
||||||
\contentsline {subsection}{\numberline {4.9.1}\IeC {\'E}nergie hydraulique}{77}%
|
\contentsline {subsection}{\numberline {4.3.1}Cin\IeC {\'e}matique}{70}%
|
||||||
\contentsline {subsubsection}{Exemple}{78}%
|
\contentsline {subsubsection}{Position}{70}%
|
||||||
\contentsline {subsubsection}{Types de turbines}{79}%
|
\contentsline {subsubsection}{Vitesse}{71}%
|
||||||
\contentsline {subsubsection}{Alternateur}{79}%
|
\contentsline {subsubsection}{Acc\IeC {\'e}l\IeC {\'e}ration}{71}%
|
||||||
\contentsline {subsubsection}{Probl\IeC {\`e}mes rencontr\IeC {\'e}s}{80}%
|
\contentsline {subsection}{\numberline {4.3.2}Dynamique}{71}%
|
||||||
\contentsline {subsection}{\numberline {4.9.2}\IeC {\'E}nergie \IeC {\'e}olienne}{80}%
|
\contentsline {subsubsection}{Premi\IeC {\`e}re loi}{71}%
|
||||||
\contentsline {subsection}{\numberline {4.9.3}\IeC {\'E}nergie solaire}{81}%
|
\contentsline {subsubsection}{Seconde loi}{71}%
|
||||||
\contentsline {subsubsection}{\IeC {\'E}nergie solaire thermique}{81}%
|
\contentsline {subsubsection}{Troisi\IeC {\`e}me loi}{71}%
|
||||||
\contentsline {subsubsection}{\IeC {\'E}nergie solaire \IeC {\'e}lectrique}{83}%
|
\contentsline {section}{\numberline {4.4}Exemples}{71}%
|
||||||
\contentsline {subsection}{\numberline {4.9.4}\IeC {\'E}nergie g\IeC {\'e}othermique}{84}%
|
\contentsline {subsection}{\numberline {4.4.1}Statique}{71}%
|
||||||
\contentsline {section}{\numberline {4.10}\IeC {\'E}nergies non renouvelables}{84}%
|
\contentsline {subsection}{\numberline {4.4.2}Plan inclin\IeC {\'e}}{72}%
|
||||||
\contentsline {subsection}{\numberline {4.10.1}\IeC {\'E}nergie nucl\IeC {\'e}aire}{85}%
|
\contentsline {subsection}{\numberline {4.4.3}Balistique}{74}%
|
||||||
\contentsline {subsubsection}{Fission}{85}%
|
\contentsline {subsection}{\numberline {4.4.4}Mouvement circulaire uniforme~: MCU}{76}%
|
||||||
\contentsline {paragraph}{D\IeC {\'e}chets radioactifs}{86}%
|
\contentsline {subsubsection}{D\IeC {\'e}finition}{76}%
|
||||||
\contentsline {paragraph}{Accidents nucl\IeC {\'e}aires}{87}%
|
\contentsline {subsubsection}{Cin\IeC {\'e}matique}{76}%
|
||||||
\contentsline {subsubsection}{Fusion}{87}%
|
\contentsline {subsubsection}{Relation importante}{77}%
|
||||||
\contentsline {subsection}{\numberline {4.10.2}\IeC {\'E}nergie de combustion~: p\IeC {\'e}trole et gaz}{87}%
|
\contentsline {subsubsection}{Dynamique}{77}%
|
||||||
\contentsline {chapter}{\numberline {5}Thermodynamique}{91}%
|
\contentsline {subsubsection}{Virages inclin\IeC {\'e}s}{77}%
|
||||||
\contentsline {section}{\numberline {5.1}Introduction}{91}%
|
\contentsline {paragraph}{Vitesses minimales}{78}%
|
||||||
\contentsline {section}{\numberline {5.2}Temp\IeC {\'e}rature}{91}%
|
\contentsline {paragraph}{Vitesses maximales}{79}%
|
||||||
\contentsline {subsection}{\numberline {5.2.1}Celsius}{91}%
|
\contentsline {subsection}{\numberline {4.4.5}Satellite en orbite g\IeC {\'e}ostationnaire}{80}%
|
||||||
\contentsline {subsection}{\numberline {5.2.2}Fahrenheit}{91}%
|
\contentsline {subsubsection}{Introduction}{80}%
|
||||||
\contentsline {subsection}{\numberline {5.2.3}Kelvin}{92}%
|
\contentsline {subsubsection}{Th\IeC {\'e}oriquement}{80}%
|
||||||
\contentsline {subsection}{\numberline {5.2.4}Agitation mol\IeC {\'e}culaire}{92}%
|
\contentsline {subsubsection}{Num\IeC {\'e}riquement}{80}%
|
||||||
\contentsline {section}{\numberline {5.3}Dilatation}{92}%
|
\contentsline {subsection}{\numberline {4.4.6}Mouvement central}{80}%
|
||||||
\contentsline {section}{\numberline {5.4}Chaleur}{93}%
|
\contentsline {subsubsection}{Mouvement kepleriens}{80}%
|
||||||
\contentsline {subsection}{\numberline {5.4.1}Chaleur sp\IeC {\'e}cifique}{93}%
|
\contentsline {subsubsection}{Loi de Kepler}{80}%
|
||||||
\contentsline {subsection}{\numberline {5.4.2}Chaleur latente}{93}%
|
\contentsline {chapter}{\numberline {5}M\IeC {\'e}canique diff\IeC {\'e}rentielle}{83}%
|
||||||
\contentsline {section}{\numberline {5.5}\IeC {\'E}nergie thermique}{94}%
|
\contentsline {section}{\numberline {5.1}Introduction}{83}%
|
||||||
\contentsline {subsection}{\numberline {5.5.1}Premier principe}{95}%
|
\contentsline {section}{\numberline {5.2}Cin\IeC {\'e}matique}{83}%
|
||||||
\contentsline {chapter}{\numberline {A}Syst\IeC {\`e}mes d'unit\IeC {\'e}s}{97}%
|
\contentsline {subsection}{\numberline {5.2.1}Exemples}{84}%
|
||||||
\contentsline {section}{\numberline {A.1}Introduction}{97}%
|
\contentsline {subsubsection}{Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e}~: MRUA}{84}%
|
||||||
\contentsline {section}{\numberline {A.2}Op\IeC {\'e}rateur d'unit\IeC {\'e}s}{97}%
|
\contentsline {subsubsection}{Port\IeC {\'e} maximum en balistique}{84}%
|
||||||
\contentsline {section}{\numberline {A.3}Analyse dimensionnelle}{98}%
|
\contentsline {section}{\numberline {5.3}Dynamique}{85}%
|
||||||
\contentsline {section}{\numberline {A.4}Les unit\IeC {\'e}s du Syst\IeC {\`e}me International}{99}%
|
\contentsline {subsection}{\numberline {5.3.1}Int\IeC {\'e}gration}{85}%
|
||||||
\contentsline {subsection}{\numberline {A.4.1}Exemple}{99}%
|
\contentsline {subsubsection}{Chute libre}{85}%
|
||||||
\contentsline {section}{\numberline {A.5}Conversions}{99}%
|
\contentsline {subsubsection}{Freinage}{85}%
|
||||||
\contentsline {section}{\numberline {A.6}Sous-multiples}{100}%
|
\contentsline {subsection}{\numberline {5.3.2}\IeC {\'E}quation diff\IeC {\'e}rentielle}{85}%
|
||||||
\contentsline {section}{\numberline {A.7}Notation scientifique}{100}%
|
\contentsline {subsubsection}{Chute dans un fluide visqueux}{85}%
|
||||||
\contentsline {section}{\numberline {A.8}R\IeC {\`e}gles de calcul}{101}%
|
\contentsline {subsubsection}{Mouvement harmonique}{87}%
|
||||||
\contentsline {chapter}{\numberline {B}Deux syst\IeC {\`e}mes de coordonn\IeC {\'e}es}{103}%
|
\contentsline {subsubsection}{Mouvement harmonique d'une masse pendante}{88}%
|
||||||
\contentsline {section}{\numberline {B.1}Le syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires}{103}%
|
\contentsline {subsubsection}{Mouvement non lin\IeC {\'e}aire}{89}%
|
||||||
\contentsline {subsection}{\numberline {B.1.1}Introduction}{103}%
|
\contentsline {chapter}{\numberline {6}Quantit\IeC {\'e} de mouvement}{91}%
|
||||||
\contentsline {subsection}{\numberline {B.1.2}Description}{103}%
|
\contentsline {section}{\numberline {6.1}Introduction}{91}%
|
||||||
\contentsline {section}{\numberline {B.2}Coordonn\IeC {\'e}es sph\IeC {\'e}riques}{103}%
|
\contentsline {section}{\numberline {6.2}Quantit\IeC {\'e} de mouvement}{91}%
|
||||||
\contentsline {subsection}{\numberline {B.2.1}Introduction}{103}%
|
\contentsline {subsection}{\numberline {6.2.1}Masse d'inertie}{91}%
|
||||||
\contentsline {subsection}{\numberline {B.2.2}Description}{103}%
|
\contentsline {section}{\numberline {6.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{92}%
|
||||||
\contentsline {subsection}{\numberline {B.2.3}Latitude et longitude}{104}%
|
\contentsline {section}{\numberline {6.4}Choc parfaitement \IeC {\'e}lastique}{92}%
|
||||||
\contentsline {chapter}{\numberline {C}Mesures de distances}{105}%
|
\contentsline {subsection}{\numberline {6.4.1}Exemple}{92}%
|
||||||
\contentsline {section}{\numberline {C.1}La taille de la Terre}{105}%
|
\contentsline {section}{\numberline {6.5}Choc parfaitement mou}{93}%
|
||||||
\contentsline {subsection}{\numberline {C.1.1}Le principe}{105}%
|
\contentsline {subsection}{\numberline {6.5.1}Exemple}{93}%
|
||||||
\contentsline {subsection}{\numberline {C.1.2}Techniquement}{106}%
|
\contentsline {section}{\numberline {6.6}choc bidimentionnel}{94}%
|
||||||
\contentsline {section}{\numberline {C.2}La taille de la Lune}{107}%
|
\contentsline {subsection}{\numberline {6.6.1}Exemple}{94}%
|
||||||
\contentsline {section}{\numberline {C.3}La distance Terre-Lune}{107}%
|
\contentsline {section}{\numberline {6.7}Impulsion}{95}%
|
||||||
\contentsline {section}{\numberline {C.4}La distance Terre-Soleil}{108}%
|
\contentsline {chapter}{\numberline {7}L'\IeC {\'e}nergie}{97}%
|
||||||
\contentsline {section}{\numberline {C.5}La distance des \IeC {\'e}toiles}{110}%
|
\contentsline {section}{\numberline {7.1}Introduction}{97}%
|
||||||
\contentsline {chapter}{\numberline {D}Travaux pratiques}{111}%
|
\contentsline {section}{\numberline {7.2}Travail}{97}%
|
||||||
\contentsline {section}{\numberline {D.1}Le rapport de laboratoire}{111}%
|
\contentsline {section}{\numberline {7.3}Puissance}{98}%
|
||||||
\contentsline {subsection}{\numberline {D.1.1}Plan d'un rapport de travail pratique}{112}%
|
\contentsline {section}{\numberline {7.4}\IeC {\'E}nergie potentielle}{98}%
|
||||||
\contentsline {subsubsection}{Pr\IeC {\'e}liminaires}{112}%
|
\contentsline {section}{\numberline {7.5}\IeC {\'E}nergie cin\IeC {\'e}tique}{99}%
|
||||||
\contentsline {subsubsection}{R\IeC {\'e}sum\IeC {\'e}}{112}%
|
\contentsline {section}{\numberline {7.6}Th\IeC {\'e}or\IeC {\`e}me de l'\IeC {\'e}nergie cin\IeC {\'e}tique}{99}%
|
||||||
\contentsline {subsubsection}{But}{112}%
|
\contentsline {section}{\numberline {7.7}Conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{99}%
|
||||||
\contentsline {subsubsection}{Th\IeC {\'e}orie}{112}%
|
\contentsline {section}{\numberline {7.8}Variation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{101}%
|
||||||
\contentsline {subsubsection}{Description de l'exp\IeC {\'e}rience}{112}%
|
\contentsline {section}{\numberline {7.9}\IeC {\'E}nergies renouvelables}{101}%
|
||||||
\contentsline {subsubsection}{R\IeC {\'e}sultats}{112}%
|
\contentsline {subsection}{\numberline {7.9.1}\IeC {\'E}nergie hydraulique}{101}%
|
||||||
\contentsline {subsubsection}{Discussion}{114}%
|
\contentsline {subsubsection}{Exemple}{102}%
|
||||||
\contentsline {subsubsection}{Conclusion}{114}%
|
\contentsline {subsubsection}{Types de turbines}{103}%
|
||||||
\contentsline {subsubsection}{Annexes}{114}%
|
\contentsline {subsubsection}{Alternateur}{103}%
|
||||||
\contentsline {section}{\numberline {D.2}La n\IeC {\'e}buleuse du Crabe}{115}%
|
\contentsline {subsubsection}{Probl\IeC {\`e}mes rencontr\IeC {\'e}s}{104}%
|
||||||
\contentsline {subsection}{\numberline {D.2.1}Introduction}{115}%
|
\contentsline {subsection}{\numberline {7.9.2}\IeC {\'E}nergie \IeC {\'e}olienne}{104}%
|
||||||
\contentsline {subsection}{\numberline {D.2.2}But du travail pratique}{115}%
|
\contentsline {subsection}{\numberline {7.9.3}\IeC {\'E}nergie solaire}{105}%
|
||||||
\contentsline {subsection}{\numberline {D.2.3}Dispositif exp\IeC {\'e}rimental}{115}%
|
\contentsline {subsubsection}{\IeC {\'E}nergie solaire thermique}{105}%
|
||||||
\contentsline {subsection}{\numberline {D.2.4}Mesures}{115}%
|
\contentsline {subsubsection}{\IeC {\'E}nergie solaire \IeC {\'e}lectrique}{107}%
|
||||||
\contentsline {subsection}{\numberline {D.2.5}R\IeC {\'e}sultats}{115}%
|
\contentsline {subsection}{\numberline {7.9.4}\IeC {\'E}nergie g\IeC {\'e}othermique}{108}%
|
||||||
\contentsline {subsection}{\numberline {D.2.6}Analyse}{115}%
|
\contentsline {section}{\numberline {7.10}\IeC {\'E}nergies non renouvelables}{108}%
|
||||||
\contentsline {section}{\numberline {D.3}Le pendule simple}{115}%
|
\contentsline {subsection}{\numberline {7.10.1}\IeC {\'E}nergie nucl\IeC {\'e}aire}{109}%
|
||||||
\contentsline {subsection}{\numberline {D.3.1}Les mesures}{115}%
|
\contentsline {subsubsection}{Fission}{109}%
|
||||||
\contentsline {subsection}{\numberline {D.3.2}Organisation des donn\IeC {\'e}es et graphiques}{117}%
|
\contentsline {paragraph}{D\IeC {\'e}chets radioactifs}{110}%
|
||||||
\contentsline {section}{\numberline {D.4}Mouvement simple~: MRU}{118}%
|
\contentsline {paragraph}{Accidents nucl\IeC {\'e}aires}{111}%
|
||||||
\contentsline {subsection}{\numberline {D.4.1}Les mesures}{118}%
|
\contentsline {subsubsection}{Fusion}{111}%
|
||||||
\contentsline {subsection}{\numberline {D.4.2}Organisation des donn\IeC {\'e}es et graphiques}{118}%
|
\contentsline {subsection}{\numberline {7.10.2}\IeC {\'E}nergie de combustion~: p\IeC {\'e}trole et gaz}{111}%
|
||||||
\contentsline {subsection}{\numberline {D.4.3}Analyse des r\IeC {\'e}sultats}{118}%
|
\contentsline {chapter}{\numberline {8}L'\IeC {\'e}nergie}{115}%
|
||||||
\contentsline {section}{\numberline {D.5}Mouvement simple~:\\MRUA}{118}%
|
\contentsline {section}{\numberline {8.1}Introduction}{115}%
|
||||||
\contentsline {subsection}{\numberline {D.5.1}But}{118}%
|
\contentsline {section}{\numberline {8.2}Le travail}{115}%
|
||||||
\contentsline {subsection}{\numberline {D.5.2}Th\IeC {\'e}orie}{118}%
|
\contentsline {subsection}{\numberline {8.2.1}Historiquement}{115}%
|
||||||
\contentsline {subsection}{\numberline {D.5.3}Les mesures}{118}%
|
\contentsline {subsection}{\numberline {8.2.2}D\IeC {\'e}finition}{116}%
|
||||||
\contentsline {subsection}{\numberline {D.5.4}Organisation des donn\IeC {\'e}es et graphiques}{119}%
|
\contentsline {subsubsection}{Travail simple}{116}%
|
||||||
\contentsline {subsection}{\numberline {D.5.5}Galil\IeC {\'e}e et le plan inclin\IeC {\'e}}{119}%
|
\contentsline {subsubsection}{Travail et produit scalaire}{116}%
|
||||||
\contentsline {section}{\numberline {D.6}La chute libre}{119}%
|
\contentsline {subsubsection}{Travail cas g\IeC {\'e}n\IeC {\'e}ral}{116}%
|
||||||
\contentsline {subsection}{\numberline {D.6.1}Cette exp\IeC {\'e}rience donnant lieu \IeC {\`a} un rapport not\IeC {\'e}, elle n'est pas d\IeC {\'e}crite.}{119}%
|
\contentsline {section}{\numberline {8.3}L'\IeC {\'e}nergie}{117}%
|
||||||
\contentsline {subsection}{\numberline {D.6.2}R\IeC {\'e}sultats}{119}%
|
\contentsline {subsection}{\numberline {8.3.1}Introduction}{117}%
|
||||||
\contentsline {section}{\numberline {D.7}Le canon horizontal}{119}%
|
\contentsline {subsection}{\numberline {8.3.2}\IeC {\'E}nergie potentielle}{117}%
|
||||||
\contentsline {section}{\numberline {D.8}Le chariot \IeC {\`a} masse pendante}{120}%
|
\contentsline {subsection}{\numberline {8.3.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{118}%
|
||||||
\contentsline {chapter}{\numberline {E}Rotations}{121}%
|
\contentsline {subsection}{\numberline {8.3.4}\IeC {\'E}nergie m\IeC {\'e}canique}{118}%
|
||||||
\contentsline {section}{\numberline {E.1}Rotation de la Terre sur elle-m\IeC {\^e}me}{121}%
|
\contentsline {subsection}{\numberline {8.3.5}Exemple}{118}%
|
||||||
\contentsline {section}{\numberline {E.2}Rotation de la Terre autour du Soleil}{121}%
|
\contentsline {section}{\numberline {8.4}Conservation de l'\IeC {\'e}nergie}{118}%
|
||||||
\contentsline {section}{\numberline {E.3}Rotation du Soleil dans la Voie Lact\IeC {\'e}e}{123}%
|
\contentsline {subsection}{\numberline {8.4.1}Introduction}{118}%
|
||||||
\contentsline {section}{\numberline {E.4}Vitesse et r\IeC {\'e}f\IeC {\'e}rentiel}{123}%
|
\contentsline {subsection}{\numberline {8.4.2}Th\IeC {\'e}or\IeC {\`e}me de conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{118}%
|
||||||
\contentsline {chapter}{\numberline {F}MRUA d\IeC {\'e}veloppements}{125}%
|
\contentsline {subsection}{\numberline {8.4.3}Exemples}{119}%
|
||||||
\contentsline {section}{\numberline {F.1}La position}{125}%
|
\contentsline {section}{\numberline {8.5}Limite du th\IeC {\'e}or\IeC {\`e}me de conservation}{120}%
|
||||||
\contentsline {section}{\numberline {F.2}Une autre relation bien pratique}{125}%
|
\contentsline {section}{\numberline {8.6}Forces conservatives}{120}%
|
||||||
\contentsline {subsection}{\numberline {F.2.1}Cin\IeC {\'e}matique}{125}%
|
\contentsline {subsection}{\numberline {8.6.1}D\IeC {\'e}finition}{120}%
|
||||||
\contentsline {subsection}{\numberline {F.2.2}\IeC {\'E}nergie}{126}%
|
\contentsline {subsection}{\numberline {8.6.2}Exemples}{120}%
|
||||||
\contentsline {chapter}{\numberline {G}Chute de la Lune}{127}%
|
\contentsline {subsubsection}{Le poids}{120}%
|
||||||
\contentsline {section}{\numberline {G.1}Introduction}{127}%
|
\contentsline {subsubsection}{Le ressort}{121}%
|
||||||
\contentsline {section}{\numberline {G.2}Acc\IeC {\'e}l\IeC {\'e}ration}{127}%
|
\contentsline {subsection}{\numberline {8.6.3}G\IeC {\'e}n\IeC {\'e}ralisation}{121}%
|
||||||
\contentsline {section}{\numberline {G.3}Force de gravitation}{128}%
|
\contentsline {subsubsection}{\IeC {\'E}nergie gravifique}{122}%
|
||||||
\contentsline {chapter}{\numberline {H}Satellite en orbite g\IeC {\'e}ostationnaire}{129}%
|
\contentsline {chapter}{\numberline {9}Physique th\IeC {\'e}orique}{125}%
|
||||||
\contentsline {section}{\numberline {H.1}Introduction}{129}%
|
\contentsline {section}{\numberline {9.1}Introduction}{125}%
|
||||||
\contentsline {section}{\numberline {H.2}Th\IeC {\'e}oriquement}{129}%
|
\contentsline {section}{\numberline {9.2}\IeC {\'E}nergie potentielle}{125}%
|
||||||
\contentsline {section}{\numberline {H.3}Num\IeC {\'e}riquement}{130}%
|
\contentsline {section}{\numberline {9.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{125}%
|
||||||
\contentsline {section}{\numberline {H.4}Loi de Kepler}{130}%
|
\contentsline {section}{\numberline {9.4}Quantit\IeC {\'e} de mouvement}{125}%
|
||||||
\contentsline {chapter}{\numberline {I}Relativit\IeC {\'e}}{131}%
|
\contentsline {section}{\numberline {9.5}Conservation de l'\IeC {\'e}nergie}{126}%
|
||||||
\contentsline {section}{\numberline {I.1}Relativit\IeC {\'e} galil\IeC {\'e}enne}{131}%
|
\contentsline {section}{\numberline {9.6}Principe de moindre action}{126}%
|
||||||
\contentsline {section}{\numberline {I.2}Transformation galil\IeC {\'e}enne}{132}%
|
\contentsline {subsection}{\numberline {9.6.1}Lagrangien}{126}%
|
||||||
\contentsline {section}{\numberline {I.3}Invariance}{133}%
|
\contentsline {subsection}{\numberline {9.6.2}Action}{126}%
|
||||||
\contentsline {section}{\numberline {I.4}Forces inertielles}{133}%
|
\contentsline {subsection}{\numberline {9.6.3}Minimalisation}{127}%
|
||||||
\contentsline {subsection}{\numberline {I.4.1}Force d'inertie}{133}%
|
\contentsline {section}{\numberline {9.7}Euler-Lagrange}{127}%
|
||||||
\contentsline {subsection}{\numberline {I.4.2}Force centrifuge}{134}%
|
\contentsline {chapter}{\numberline {10}Thermodynamique}{129}%
|
||||||
\contentsline {chapter}{\numberline {J}Mar\IeC {\'e}es}{135}%
|
\contentsline {section}{\numberline {10.1}Introduction}{129}%
|
||||||
\contentsline {section}{\numberline {J.1}Introduction}{135}%
|
\contentsline {section}{\numberline {10.2}Temp\IeC {\'e}rature}{129}%
|
||||||
\contentsline {section}{\numberline {J.2}Centre de gravit\IeC {\'e}}{135}%
|
\contentsline {subsection}{\numberline {10.2.1}Celsius}{129}%
|
||||||
\contentsline {section}{\numberline {J.3}Force d'inertie}{136}%
|
\contentsline {subsection}{\numberline {10.2.2}Fahrenheit}{129}%
|
||||||
\contentsline {subsection}{\numberline {J.3.1}Vitesse angulaire}{136}%
|
\contentsline {subsection}{\numberline {10.2.3}Kelvin}{130}%
|
||||||
\contentsline {subsection}{\numberline {J.3.2}Force d'inertie}{136}%
|
\contentsline {subsection}{\numberline {10.2.4}Agitation mol\IeC {\'e}culaire}{130}%
|
||||||
\contentsline {section}{\numberline {J.4}Poids relatif}{137}%
|
\contentsline {section}{\numberline {10.3}Dilatation}{130}%
|
||||||
\contentsline {section}{\numberline {J.5}Analyse diff\IeC {\'e}rentielle}{137}%
|
\contentsline {section}{\numberline {10.4}Chaleur}{131}%
|
||||||
\contentsline {section}{\numberline {J.6}Autres rythmes}{137}%
|
\contentsline {subsection}{\numberline {10.4.1}Chaleur sp\IeC {\'e}cifique}{131}%
|
||||||
\contentsline {subsection}{\numberline {J.6.1}D\IeC {\'e}calages}{138}%
|
\contentsline {subsection}{\numberline {10.4.2}Chaleur latente}{131}%
|
||||||
\contentsline {subsection}{\numberline {J.6.2}Mar\IeC {\'e}es de vives et mortes eaux}{138}%
|
\contentsline {section}{\numberline {10.5}\IeC {\'E}nergie thermique}{132}%
|
||||||
\contentsline {subsection}{\numberline {J.6.3}Mar\IeC {\'e}es d'\IeC {\'e}quinoxes}{138}%
|
\contentsline {subsection}{\numberline {10.5.1}Premier principe}{133}%
|
||||||
\contentsline {subsection}{\numberline {J.6.4}Mar\IeC {\'e}es de p\IeC {\'e}rig\IeC {\'e}e et p\IeC {\'e}rih\IeC {\'e}lie}{139}%
|
\contentsline {chapter}{\numberline {11}Thermodynamique}{135}%
|
||||||
\contentsline {subsection}{\numberline {J.6.5}Mar\IeC {\'e}es de d\IeC {\'e}clinaison}{139}%
|
\contentsline {section}{\numberline {11.1}Temp\IeC {\'e}rature et dilatation}{135}%
|
||||||
\contentsline {subsection}{\numberline {J.6.6}Retards et mar\IeC {\'e}es c\IeC {\^o}ti\IeC {\`e}res}{139}%
|
\contentsline {subsection}{\numberline {11.1.1}Temp\IeC {\'e}rature}{135}%
|
||||||
\contentsline {section}{\numberline {J.7}Limite de Roche}{139}%
|
\contentsline {subsection}{\numberline {11.1.2}Dilatation}{135}%
|
||||||
\contentsline {subsection}{\numberline {J.7.1}Mod\IeC {\`e}le simplifi\IeC {\'e}}{140}%
|
\contentsline {section}{\numberline {11.2}Chaleurs sp\IeC {\'e}cifique et latente}{137}%
|
||||||
\contentsline {subsection}{\numberline {J.7.2}Exemples}{141}%
|
\contentsline {subsection}{\numberline {11.2.1}Introduction}{137}%
|
||||||
\contentsline {chapter}{\numberline {K}\IeC {\'E}nergies}{143}%
|
\contentsline {subsection}{\numberline {11.2.2}Chaleur sp\IeC {\'e}cifique}{137}%
|
||||||
\contentsline {section}{\numberline {K.1}Introduction}{143}%
|
\contentsline {subsubsection}{Chaleur massique}{137}%
|
||||||
\contentsline {section}{\numberline {K.2}\IeC {\'E}nergie hydraulique}{143}%
|
\contentsline {subsubsection}{Capacit\IeC {\'e} thermique}{138}%
|
||||||
\contentsline {section}{\numberline {K.3}\IeC {\'E}nergie \IeC {\'e}olienne}{144}%
|
\contentsline {subsubsection}{Notion de mole}{138}%
|
||||||
\contentsline {subsection}{\numberline {K.3.1}R\IeC {\`e}gle de Betz}{144}%
|
\contentsline {subsubsection}{Chaleur molaire}{138}%
|
||||||
\contentsline {subsection}{\numberline {K.3.2}\IeC {\'E}oliennes}{145}%
|
\contentsline {subsubsection}{Relation entre chaleur massique et molaire}{139}%
|
||||||
\contentsline {subsubsection}{\IeC {\'E}olienne de Collonges-Dor\IeC {\'e}naz}{145}%
|
\contentsline {subsubsection}{Chaleur latente}{139}%
|
||||||
\contentsline {subsubsection}{\IeC {\'E}oliennes du Mont Soleil (Jura suisse)}{145}%
|
\contentsline {subsubsection}{\IeC {\'E}vaporation}{140}%
|
||||||
\contentsline {section}{\numberline {K.4}G\IeC {\'e}othermie}{145}%
|
\contentsline {subsection}{\numberline {11.2.3}Bilan thermique}{140}%
|
||||||
\contentsline {section}{\numberline {K.5}\IeC {\'E}nergie de combustion des d\IeC {\'e}chets}{146}%
|
\contentsline {section}{\numberline {11.3}Loi des gaz parfaits}{141}%
|
||||||
\contentsline {chapter}{\numberline {L}Exercices}{147}%
|
\contentsline {subsection}{\numberline {11.3.1}\IeC {\'E}quation d'\IeC {\'e}tat}{141}%
|
||||||
\contentsline {section}{\numberline {L.1}Probl\IeC {\`e}mes}{147}%
|
\contentsline {subsubsection}{Pression}{141}%
|
||||||
\contentsline {subsection}{\numberline {L.1.1}Relatifs \IeC {\`a} la conversion d'unit\IeC {\'e}s et \IeC {\`a} la notation scientifique}{147}%
|
\contentsline {subsubsection}{\IeC {\'E}tat d'un gaz parfait}{141}%
|
||||||
\contentsline {subsection}{\numberline {L.1.2}Relatifs aux notions de d\IeC {\'e}placement, position et distance parcourue}{147}%
|
\contentsline {subsubsection}{Approche intuitive}{141}%
|
||||||
\contentsline {subsection}{\numberline {L.1.3}Relatifs \IeC {\`a} la notion de vitesse}{148}%
|
\contentsline {subsubsection}{Approche mol\IeC {\'e}culaire}{142}%
|
||||||
\contentsline {subsection}{\numberline {L.1.4}Relatif \IeC {\`a} la notion d'acc\IeC {\'e}l\IeC {\'e}ration}{148}%
|
\contentsline {subsection}{\numberline {11.3.2}Gaz parfait}{143}%
|
||||||
\contentsline {subsection}{\numberline {L.1.5}Relatif au MRU}{149}%
|
\contentsline {section}{\numberline {11.4}Premier principe}{143}%
|
||||||
\contentsline {subsection}{\numberline {L.1.6}Relatif au MRUA}{149}%
|
\contentsline {subsection}{\numberline {11.4.1}Chaleur}{143}%
|
||||||
\contentsline {subsection}{\numberline {L.1.7}Relatifs \IeC {\`a} la physique aristot\IeC {\'e}licienne}{150}%
|
\contentsline {subsection}{\numberline {11.4.2}Travail}{144}%
|
||||||
\contentsline {subsection}{\numberline {L.1.8}Relatifs \IeC {\`a} la physique newtonienne}{150}%
|
\contentsline {subsection}{\numberline {11.4.3}\IeC {\'E}nergie interne}{144}%
|
||||||
\contentsline {subsection}{\numberline {L.1.9}Relatifs aux forces}{151}%
|
\contentsline {subsubsection}{\IeC {\'E}quipartition de l'\IeC {\'e}nergie}{145}%
|
||||||
\contentsline {subsection}{\numberline {L.1.10}Relatifs \IeC {\`a} l'\IeC {\'e}nergie}{152}%
|
\contentsline {subsection}{\numberline {11.4.4}Premier principe}{145}%
|
||||||
\contentsline {subsection}{\numberline {L.1.11}Relatifs \IeC {\`a} la conservation de l'\IeC {\'e}nergie}{152}%
|
\contentsline {subsection}{\numberline {11.4.5}Changements d'\IeC {\'e}tats}{145}%
|
||||||
\contentsline {subsection}{\numberline {L.1.12}Relatifs \IeC {\`a} l'\IeC {\'e}nergie hydraulique}{153}%
|
\contentsline {subsubsection}{Transformation isobare}{146}%
|
||||||
\contentsline {subsection}{\numberline {L.1.13}Relatifs \IeC {\`a} l'\IeC {\'e}nergie \IeC {\'e}olienne}{153}%
|
\contentsline {subsubsection}{Transformation isochore}{146}%
|
||||||
\contentsline {subsection}{\numberline {L.1.14}Relatifs \IeC {\`a} l'\IeC {\'e}nergie solaire}{153}%
|
\contentsline {subsubsection}{Transformation isotherme}{147}%
|
||||||
\contentsline {section}{\numberline {L.2}Solutions}{154}%
|
\contentsline {subsubsection}{Transformation adiabatique}{148}%
|
||||||
|
\contentsline {subsection}{\numberline {11.4.6}Chaleurs sp\IeC {\'e}cifiques}{149}%
|
||||||
|
\contentsline {section}{\numberline {11.5}Machines thermiques}{150}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.1}Machine simple}{150}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.2}Moteur \IeC {\`a} explosion}{152}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.3}Moteur Diesel}{154}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.4}Machine de Stirling}{156}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.5}Climatiseur}{156}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.6}R\IeC {\'e}frig\IeC {\'e}rateur}{156}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.7}Pompe \IeC {\`a} chaleur}{156}%
|
||||||
|
\contentsline {subsection}{\numberline {11.5.8}Cycle de Carnot}{156}%
|
||||||
|
\contentsline {section}{\numberline {11.6}Thermodynamique statistique}{157}%
|
||||||
|
\contentsline {section}{\numberline {11.7}Second principe}{158}%
|
||||||
|
\contentsline {chapter}{\numberline {A}Syst\IeC {\`e}mes d'unit\IeC {\'e}s}{159}%
|
||||||
|
\contentsline {section}{\numberline {A.1}Introduction}{159}%
|
||||||
|
\contentsline {section}{\numberline {A.2}Op\IeC {\'e}rateur d'unit\IeC {\'e}s}{159}%
|
||||||
|
\contentsline {section}{\numberline {A.3}Analyse dimensionnelle}{160}%
|
||||||
|
\contentsline {section}{\numberline {A.4}Les unit\IeC {\'e}s du Syst\IeC {\`e}me International}{161}%
|
||||||
|
\contentsline {subsection}{\numberline {A.4.1}Exemple}{161}%
|
||||||
|
\contentsline {section}{\numberline {A.5}Conversions}{161}%
|
||||||
|
\contentsline {section}{\numberline {A.6}Sous-multiples}{162}%
|
||||||
|
\contentsline {section}{\numberline {A.7}Notation scientifique}{162}%
|
||||||
|
\contentsline {section}{\numberline {A.8}R\IeC {\`e}gles de calcul}{163}%
|
||||||
|
\contentsline {chapter}{\numberline {B}Deux syst\IeC {\`e}mes de coordonn\IeC {\'e}es}{165}%
|
||||||
|
\contentsline {section}{\numberline {B.1}Le syst\IeC {\`e}me de coordonn\IeC {\'e}es circulaires}{165}%
|
||||||
|
\contentsline {subsection}{\numberline {B.1.1}Introduction}{165}%
|
||||||
|
\contentsline {subsection}{\numberline {B.1.2}Description}{165}%
|
||||||
|
\contentsline {section}{\numberline {B.2}Coordonn\IeC {\'e}es sph\IeC {\'e}riques}{165}%
|
||||||
|
\contentsline {subsection}{\numberline {B.2.1}Introduction}{165}%
|
||||||
|
\contentsline {subsection}{\numberline {B.2.2}Description}{165}%
|
||||||
|
\contentsline {subsection}{\numberline {B.2.3}Latitude et longitude}{166}%
|
||||||
|
\contentsline {chapter}{\numberline {C}Mesures de distances}{167}%
|
||||||
|
\contentsline {section}{\numberline {C.1}La taille de la Terre}{167}%
|
||||||
|
\contentsline {subsection}{\numberline {C.1.1}Le principe}{167}%
|
||||||
|
\contentsline {subsection}{\numberline {C.1.2}Techniquement}{168}%
|
||||||
|
\contentsline {section}{\numberline {C.2}La taille de la Lune}{169}%
|
||||||
|
\contentsline {section}{\numberline {C.3}La distance Terre-Lune}{169}%
|
||||||
|
\contentsline {section}{\numberline {C.4}La distance Terre-Soleil}{170}%
|
||||||
|
\contentsline {section}{\numberline {C.5}La distance des \IeC {\'e}toiles}{172}%
|
||||||
|
\contentsline {chapter}{\numberline {D}Travaux pratiques}{173}%
|
||||||
|
\contentsline {section}{\numberline {D.1}Le rapport de laboratoire}{173}%
|
||||||
|
\contentsline {subsection}{\numberline {D.1.1}Plan d'un rapport de travail pratique}{174}%
|
||||||
|
\contentsline {subsubsection}{Pr\IeC {\'e}liminaires}{174}%
|
||||||
|
\contentsline {subsubsection}{R\IeC {\'e}sum\IeC {\'e}}{174}%
|
||||||
|
\contentsline {subsubsection}{But}{174}%
|
||||||
|
\contentsline {subsubsection}{Th\IeC {\'e}orie}{174}%
|
||||||
|
\contentsline {subsubsection}{Description de l'exp\IeC {\'e}rience}{174}%
|
||||||
|
\contentsline {subsubsection}{R\IeC {\'e}sultats}{174}%
|
||||||
|
\contentsline {subsubsection}{Discussion}{176}%
|
||||||
|
\contentsline {subsubsection}{Conclusion}{176}%
|
||||||
|
\contentsline {subsubsection}{Annexes}{176}%
|
||||||
|
\contentsline {section}{\numberline {D.2}La n\IeC {\'e}buleuse du Crabe}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.1}Introduction}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.2}But du travail pratique}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.3}Dispositif exp\IeC {\'e}rimental}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.4}Mesures}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.5}R\IeC {\'e}sultats}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.2.6}Analyse}{177}%
|
||||||
|
\contentsline {section}{\numberline {D.3}Le pendule simple}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.3.1}Les mesures}{177}%
|
||||||
|
\contentsline {subsection}{\numberline {D.3.2}Organisation des donn\IeC {\'e}es et graphiques}{179}%
|
||||||
|
\contentsline {section}{\numberline {D.4}Mouvement simple~: MRU}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.4.1}Les mesures}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.4.2}Organisation des donn\IeC {\'e}es et graphiques}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.4.3}Analyse des r\IeC {\'e}sultats}{180}%
|
||||||
|
\contentsline {section}{\numberline {D.5}Mouvement simple~:\\MRUA}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.5.1}But}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.5.2}Th\IeC {\'e}orie}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.5.3}Les mesures}{180}%
|
||||||
|
\contentsline {subsection}{\numberline {D.5.4}Organisation des donn\IeC {\'e}es et graphiques}{181}%
|
||||||
|
\contentsline {subsection}{\numberline {D.5.5}Galil\IeC {\'e}e et le plan inclin\IeC {\'e}}{181}%
|
||||||
|
\contentsline {section}{\numberline {D.6}La chute libre}{181}%
|
||||||
|
\contentsline {subsection}{\numberline {D.6.1}Cette exp\IeC {\'e}rience donnant lieu \IeC {\`a} un rapport not\IeC {\'e}, elle n'est pas d\IeC {\'e}crite.}{181}%
|
||||||
|
\contentsline {subsection}{\numberline {D.6.2}R\IeC {\'e}sultats}{181}%
|
||||||
|
\contentsline {section}{\numberline {D.7}Le canon horizontal}{181}%
|
||||||
|
\contentsline {section}{\numberline {D.8}Le chariot \IeC {\`a} masse pendante}{182}%
|
||||||
|
\contentsline {chapter}{\numberline {E}Rotations}{183}%
|
||||||
|
\contentsline {section}{\numberline {E.1}Rotation de la Terre sur elle-m\IeC {\^e}me}{183}%
|
||||||
|
\contentsline {section}{\numberline {E.2}Rotation de la Terre autour du Soleil}{183}%
|
||||||
|
\contentsline {section}{\numberline {E.3}Rotation du Soleil dans la Voie Lact\IeC {\'e}e}{185}%
|
||||||
|
\contentsline {section}{\numberline {E.4}Vitesse et r\IeC {\'e}f\IeC {\'e}rentiel}{185}%
|
||||||
|
\contentsline {chapter}{\numberline {F}MRUA d\IeC {\'e}veloppements}{187}%
|
||||||
|
\contentsline {section}{\numberline {F.1}La position}{187}%
|
||||||
|
\contentsline {section}{\numberline {F.2}Une autre relation bien pratique}{187}%
|
||||||
|
\contentsline {subsection}{\numberline {F.2.1}Cin\IeC {\'e}matique}{187}%
|
||||||
|
\contentsline {subsection}{\numberline {F.2.2}\IeC {\'E}nergie}{188}%
|
||||||
|
\contentsline {chapter}{\numberline {G}Chute de la Lune}{189}%
|
||||||
|
\contentsline {section}{\numberline {G.1}Introduction}{189}%
|
||||||
|
\contentsline {section}{\numberline {G.2}Acc\IeC {\'e}l\IeC {\'e}ration}{189}%
|
||||||
|
\contentsline {section}{\numberline {G.3}Force de gravitation}{190}%
|
||||||
|
\contentsline {chapter}{\numberline {H}Satellite en orbite g\IeC {\'e}ostationnaire}{191}%
|
||||||
|
\contentsline {section}{\numberline {H.1}Introduction}{191}%
|
||||||
|
\contentsline {section}{\numberline {H.2}Th\IeC {\'e}oriquement}{191}%
|
||||||
|
\contentsline {section}{\numberline {H.3}Num\IeC {\'e}riquement}{192}%
|
||||||
|
\contentsline {section}{\numberline {H.4}Loi de Kepler}{192}%
|
||||||
|
\contentsline {chapter}{\numberline {I}Relativit\IeC {\'e}}{193}%
|
||||||
|
\contentsline {section}{\numberline {I.1}Relativit\IeC {\'e} galil\IeC {\'e}enne}{193}%
|
||||||
|
\contentsline {section}{\numberline {I.2}Transformation galil\IeC {\'e}enne}{194}%
|
||||||
|
\contentsline {section}{\numberline {I.3}Invariance}{195}%
|
||||||
|
\contentsline {section}{\numberline {I.4}Forces inertielles}{195}%
|
||||||
|
\contentsline {subsection}{\numberline {I.4.1}Force d'inertie}{195}%
|
||||||
|
\contentsline {subsection}{\numberline {I.4.2}Force centrifuge}{196}%
|
||||||
|
\contentsline {chapter}{\numberline {J}Mar\IeC {\'e}es}{197}%
|
||||||
|
\contentsline {section}{\numberline {J.1}Introduction}{197}%
|
||||||
|
\contentsline {section}{\numberline {J.2}Centre de gravit\IeC {\'e}}{197}%
|
||||||
|
\contentsline {section}{\numberline {J.3}Force d'inertie}{198}%
|
||||||
|
\contentsline {subsection}{\numberline {J.3.1}Vitesse angulaire}{198}%
|
||||||
|
\contentsline {subsection}{\numberline {J.3.2}Force d'inertie}{198}%
|
||||||
|
\contentsline {section}{\numberline {J.4}Poids relatif}{199}%
|
||||||
|
\contentsline {section}{\numberline {J.5}Analyse diff\IeC {\'e}rentielle}{199}%
|
||||||
|
\contentsline {section}{\numberline {J.6}Autres rythmes}{199}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.1}D\IeC {\'e}calages}{200}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.2}Mar\IeC {\'e}es de vives et mortes eaux}{200}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.3}Mar\IeC {\'e}es d'\IeC {\'e}quinoxes}{200}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.4}Mar\IeC {\'e}es de p\IeC {\'e}rig\IeC {\'e}e et p\IeC {\'e}rih\IeC {\'e}lie}{201}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.5}Mar\IeC {\'e}es de d\IeC {\'e}clinaison}{201}%
|
||||||
|
\contentsline {subsection}{\numberline {J.6.6}Retards et mar\IeC {\'e}es c\IeC {\^o}ti\IeC {\`e}res}{201}%
|
||||||
|
\contentsline {section}{\numberline {J.7}Limite de Roche}{201}%
|
||||||
|
\contentsline {subsection}{\numberline {J.7.1}Mod\IeC {\`e}le simplifi\IeC {\'e}}{202}%
|
||||||
|
\contentsline {subsection}{\numberline {J.7.2}Exemples}{203}%
|
||||||
|
\contentsline {chapter}{\numberline {K}\IeC {\'E}nergies}{205}%
|
||||||
|
\contentsline {section}{\numberline {K.1}Introduction}{205}%
|
||||||
|
\contentsline {section}{\numberline {K.2}\IeC {\'E}nergie hydraulique}{205}%
|
||||||
|
\contentsline {section}{\numberline {K.3}\IeC {\'E}nergie \IeC {\'e}olienne}{206}%
|
||||||
|
\contentsline {subsection}{\numberline {K.3.1}R\IeC {\`e}gle de Betz}{206}%
|
||||||
|
\contentsline {subsection}{\numberline {K.3.2}\IeC {\'E}oliennes}{207}%
|
||||||
|
\contentsline {subsubsection}{\IeC {\'E}olienne de Collonges-Dor\IeC {\'e}naz}{207}%
|
||||||
|
\contentsline {subsubsection}{\IeC {\'E}oliennes du Mont Soleil (Jura suisse)}{207}%
|
||||||
|
\contentsline {section}{\numberline {K.4}G\IeC {\'e}othermie}{207}%
|
||||||
|
\contentsline {section}{\numberline {K.5}\IeC {\'E}nergie de combustion des d\IeC {\'e}chets}{208}%
|
||||||
|
\contentsline {chapter}{\numberline {L}Exercices}{209}%
|
||||||
|
\contentsline {section}{\numberline {L.1}Probl\IeC {\`e}mes}{209}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.1}Relatifs \IeC {\`a} la conversion d'unit\IeC {\'e}s et \IeC {\`a} la notation scientifique}{209}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.2}Relatifs aux notions de d\IeC {\'e}placement, position et distance parcourue}{209}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.3}Relatifs \IeC {\`a} la notion de vitesse}{210}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.4}Relatif \IeC {\`a} la notion d'acc\IeC {\'e}l\IeC {\'e}ration}{210}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.5}Relatif au MRU}{211}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.6}Relatif au MRUA}{211}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.7}Relatifs \IeC {\`a} la physique aristot\IeC {\'e}licienne}{212}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.8}Relatifs \IeC {\`a} la physique newtonienne}{212}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.9}Relatifs aux forces}{214}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.10}Relatifs \IeC {\`a} l'\IeC {\'e}nergie}{216}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.11}Relatifs \IeC {\`a} la conservation de l'\IeC {\'e}nergie}{216}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.12}Relatifs \IeC {\`a} l'\IeC {\'e}nergie hydraulique}{217}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.13}Relatifs \IeC {\`a} l'\IeC {\'e}nergie \IeC {\'e}olienne}{217}%
|
||||||
|
\contentsline {subsection}{\numberline {L.1.14}Relatifs \IeC {\`a} l'\IeC {\'e}nergie solaire}{217}%
|
||||||
|
\contentsline {section}{\numberline {L.2}Solutions}{218}%
|
||||||
|
\contentsline {section}{\numberline {L.3}Solutions OS}{233}%
|
||||||
|
\contentsline {chapter}{\numberline {M}Ordre de grandeur, erreur et incertitudes}{245}%
|
||||||
|
\contentsline {section}{\numberline {M.1}Ordre de grandeur}{245}%
|
||||||
|
\contentsline {subsection}{\numberline {M.1.1}Chiffres significatifs}{245}%
|
||||||
|
\contentsline {subsection}{\numberline {M.1.2}Ordre de grandeur}{245}%
|
||||||
|
\contentsline {section}{\numberline {M.2}\IeC {\'E}cart et erreur}{246}%
|
||||||
|
\contentsline {section}{\numberline {M.3}Incertitude}{248}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.1}Addition/soustraction}{248}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.2}Multiplication par un entier}{249}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.3}Multiplication/division}{249}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.4}Puissance}{250}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.5}R\IeC {\'e}sum\IeC {\'e}}{250}%
|
||||||
|
\contentsline {subsection}{\numberline {M.3.6}Exemples}{251}%
|
||||||
|
|||||||
@ -1,105 +1,105 @@
|
|||||||
\relax
|
\relax
|
||||||
\citation{EL99}
|
\citation{EL99}
|
||||||
\newlabel{dynamique}{{3}{51}}
|
\newlabel{dynamique}{{3}{47}}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {3}La m\IeC {\'e}canique}{51}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {3}La m\IeC {\'e}canique}{47}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {3.1}La \FB@og m\IeC {\'e}canique\fg {} d'Aristote}{51}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {3.1}La \FB@og m\IeC {\'e}canique\fg {} d'Aristote}{47}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.1}Introduction}{51}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.1}Introduction}{47}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.2}Platon}{51}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.2}Platon}{47}\protected@file@percent }
|
||||||
\citation{GSJ05}
|
\citation{GSJ05}
|
||||||
\newlabel{Aristote}{{3.1.3}{52}}
|
\newlabel{Aristote}{{3.1.3}{48}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.3}Aristote}{52}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1.3}Aristote}{48}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Cin\IeC {\'e}matique}{52}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Cin\IeC {\'e}matique}{48}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Dynamique}{52}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Dynamique}{48}\protected@file@percent }
|
||||||
\citation{SH03}
|
\citation{SH03}
|
||||||
\citation{BM85}
|
\citation{BM85}
|
||||||
\citation{BM85}
|
\citation{BM85}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {3.2}M\IeC {\'e}canique de Newton}{55}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {3.2}M\IeC {\'e}canique de Newton}{51}\protected@file@percent }
|
||||||
\newlabel{mecaniquenewton}{{3.2}{55}}
|
\newlabel{mecaniquenewton}{{3.2}{51}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.1}Introduction}{55}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.1}Introduction}{51}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.2}M\IeC {\'e}canique}{55}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.2}M\IeC {\'e}canique}{51}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Les trois lois de Newton}{55}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Les trois lois de Newton}{51}\protected@file@percent }
|
||||||
\citation{BM85}
|
\citation{BM85}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Force ext\IeC {\'e}rieure}{56}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Force ext\IeC {\'e}rieure}{52}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemples}{57}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemples}{53}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.3}Types de forces}{57}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2.3}Types de forces}{53}\protected@file@percent }
|
||||||
\citation{SH03}
|
\citation{SH03}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.1}{\ignorespaces La balance de Cavendish}}{58}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.1}{\ignorespaces La balance de Cavendish}}{54}\protected@file@percent }
|
||||||
\newlabel{balancedecavendish}{{3.1}{58}}
|
\newlabel{balancedecavendish}{{3.1}{54}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Loi de la gravitation universelle}{58}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Loi de la gravitation universelle}{54}\protected@file@percent }
|
||||||
\newlabel{gravitationuniverselle}{{3.2.3}{58}}
|
\newlabel{gravitationuniverselle}{{3.2.3}{54}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Le poids}{58}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Le poids}{54}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.2}{\ignorespaces Loi de la gravitation universelle.\relax }}{59}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.2}{\ignorespaces Loi de la gravitation universelle.\relax }}{55}\protected@file@percent }
|
||||||
\newlabel{gravitation}{{3.2}{59}}
|
\newlabel{gravitation}{{3.2}{55}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Exemple}{59}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Exemple}{55}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Masse et poids}{60}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Masse et poids}{56}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Poids apparent}{60}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Poids apparent}{56}\protected@file@percent }
|
||||||
\newlabel{poidsapparent}{{3.2.3}{60}}
|
\newlabel{poidsapparent}{{3.2.3}{56}}
|
||||||
\newlabel{a<0}{{3.3(a)}{61}}
|
\newlabel{a<0}{{3.3(a)}{57}}
|
||||||
\newlabel{sub@a<0}{{(a)}{61}}
|
\newlabel{sub@a<0}{{(a)}{57}}
|
||||||
\newlabel{a=0}{{3.3(b)}{61}}
|
\newlabel{a=0}{{3.3(b)}{57}}
|
||||||
\newlabel{sub@a=0}{{(b)}{61}}
|
\newlabel{sub@a=0}{{(b)}{57}}
|
||||||
\newlabel{a>0}{{3.3(c)}{61}}
|
\newlabel{a>0}{{3.3(c)}{57}}
|
||||||
\newlabel{sub@a>0}{{(c)}{61}}
|
\newlabel{sub@a>0}{{(c)}{57}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.3}{\ignorespaces Poids apparent\relax }}{61}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.3}{\ignorespaces Poids apparent\relax }}{57}\protected@file@percent }
|
||||||
\newlabel{3ascenseur}{{3.3}{61}}
|
\newlabel{3ascenseur}{{3.3}{57}}
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {a<0}}}{61}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {a<0}}}{57}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {a=0}}}{61}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {a=0}}}{57}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {a>0}}}{61}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {a>0}}}{57}\protected@file@percent }
|
||||||
\newlabel{eqa=0}{{3.10}{61}}
|
\newlabel{eqa=0}{{3.10}{57}}
|
||||||
\newlabel{eqa>0}{{3.11}{61}}
|
\newlabel{eqa>0}{{3.11}{57}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Gravitation et MCU}{62}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Gravitation et MCU}{58}\protected@file@percent }
|
||||||
\newlabel{accmcu}{{3.2.3}{62}}
|
\newlabel{accmcu}{{3.2.3}{58}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.4}{\ignorespaces La sensation des mouvements}}{62}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.4}{\ignorespaces La sensation des mouvements}}{58}\protected@file@percent }
|
||||||
\newlabel{mcun}{{3.4}{62}}
|
\newlabel{mcun}{{3.4}{58}}
|
||||||
\newlabel{inertiel}{{3.12}{63}}
|
\newlabel{inertiel}{{3.12}{59}}
|
||||||
\newlabel{centrifugenoninertiel}{{3.13}{63}}
|
\newlabel{centrifugenoninertiel}{{3.13}{59}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.5}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{63}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.5}{\ignorespaces L'id\IeC {\'e}e de la chute de la Lune Illustration des Principia.\relax }}{59}\protected@file@percent }
|
||||||
\newlabel{chuteprincipia}{{3.5}{63}}
|
\newlabel{chuteprincipia}{{3.5}{59}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Troisi\IeC {\`e}me loi de Kepler}{63}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Troisi\IeC {\`e}me loi de Kepler}{59}\protected@file@percent }
|
||||||
\newlabel{gravcentri}{{3.14}{64}}
|
\newlabel{gravcentri}{{3.14}{60}}
|
||||||
\newlabel{vitcirc}{{3.15}{64}}
|
\newlabel{vitcirc}{{3.15}{60}}
|
||||||
\newlabel{troiskeplernewton}{{3.16}{64}}
|
\newlabel{troiskeplernewton}{{3.16}{60}}
|
||||||
\newlabel{masselunekepler}{{3.17}{64}}
|
\newlabel{masselunekepler}{{3.17}{60}}
|
||||||
\citation{OG04}
|
\citation{OG04}
|
||||||
\citation{BS07}
|
\citation{BS07}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Les mar\IeC {\'e}es}{65}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Les mar\IeC {\'e}es}{61}\protected@file@percent }
|
||||||
\newlabel{paramarees}{{3.2.3}{65}}
|
\newlabel{paramarees}{{3.2.3}{61}}
|
||||||
\newlabel{logiquemaisfaux}{{3.6(a)}{65}}
|
\newlabel{logiquemaisfaux}{{3.6(a)}{61}}
|
||||||
\newlabel{sub@logiquemaisfaux}{{(a)}{65}}
|
\newlabel{sub@logiquemaisfaux}{{(a)}{61}}
|
||||||
\newlabel{lecasreel}{{3.6(b)}{65}}
|
\newlabel{lecasreel}{{3.6(b)}{61}}
|
||||||
\newlabel{sub@lecasreel}{{(b)}{65}}
|
\newlabel{sub@lecasreel}{{(b)}{61}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.6}{\ignorespaces Pleines et basses mers\relax }}{65}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.6}{\ignorespaces Pleines et basses mers\relax }}{61}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Logique mais faux}}}{65}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Logique mais faux}}}{61}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Le cas r\IeC {\'e}el}}}{65}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Le cas r\IeC {\'e}el}}}{61}\protected@file@percent }
|
||||||
\newlabel{rapportlunesoleil}{{3.18}{66}}
|
\newlabel{rapportlunesoleil}{{3.18}{62}}
|
||||||
\citation{GC88}
|
\citation{GC88}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.7}{\ignorespaces Syst\IeC {\`e}me Terre-Lune}}{67}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.7}{\ignorespaces Syst\IeC {\`e}me Terre-Lune}}{63}\protected@file@percent }
|
||||||
\newlabel{pleinebassemercg}{{3.7}{67}}
|
\newlabel{pleinebassemercg}{{3.7}{63}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.8}{\ignorespaces Construction de Proctor}}{67}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.8}{\ignorespaces Construction de Proctor}}{63}\protected@file@percent }
|
||||||
\newlabel{constructionproctor}{{3.8}{67}}
|
\newlabel{constructionproctor}{{3.8}{63}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.9}{\ignorespaces Force de mar\IeC {\'e}e}}{68}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.9}{\ignorespaces Force de mar\IeC {\'e}e}}{64}\protected@file@percent }
|
||||||
\newlabel{mareechampforce}{{3.9}{68}}
|
\newlabel{mareechampforce}{{3.9}{64}}
|
||||||
\newlabel{eqmareevect}{{3.19}{68}}
|
\newlabel{eqmareevect}{{3.19}{64}}
|
||||||
\newlabel{eqmaree}{{3.20}{68}}
|
\newlabel{eqmaree}{{3.20}{64}}
|
||||||
\newlabel{rapportjuste}{{3.23}{69}}
|
\newlabel{rapportjuste}{{3.23}{65}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Le frottement}{69}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Le frottement}{65}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.10}{\ignorespaces La force de frottement\relax }}{69}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.10}{\ignorespaces La force de frottement\relax }}{65}\protected@file@percent }
|
||||||
\newlabel{forcefrott}{{3.10}{69}}
|
\newlabel{forcefrott}{{3.10}{65}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.11}{\ignorespaces Freins de wagon\relax }}{70}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.11}{\ignorespaces Freins de wagon\relax }}{66}\protected@file@percent }
|
||||||
\newlabel{freindewagon}{{3.11}{70}}
|
\newlabel{freindewagon}{{3.11}{66}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Exemple}{70}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Exemple}{66}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.12}{\ignorespaces Essieu de wagon\relax }}{70}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.12}{\ignorespaces Essieu de wagon\relax }}{66}\protected@file@percent }
|
||||||
\newlabel{essieudewagon}{{3.12}{70}}
|
\newlabel{essieudewagon}{{3.12}{66}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.13}{\ignorespaces Force \IeC {\'e}lastique d'un ressort\relax }}{70}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.13}{\ignorespaces Force \IeC {\'e}lastique d'un ressort\relax }}{66}\protected@file@percent }
|
||||||
\newlabel{ressort}{{3.13}{70}}
|
\newlabel{ressort}{{3.13}{66}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{La force d'un ressort}{70}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{La force d'un ressort}{66}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Exemple}{70}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Exemple}{66}\protected@file@percent }
|
||||||
\newlabel{RF2}{72}
|
\newlabel{RF2}{68}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {3.14}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de m\IeC {\'e}canique\relax }}{72}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {3.14}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de m\IeC {\'e}canique\relax }}{68}\protected@file@percent }
|
||||||
\@setckpt{Dynamique/Dynamique}{
|
\@setckpt{Dynamique/Dynamique}{
|
||||||
\setcounter{page}{73}
|
\setcounter{page}{69}
|
||||||
\setcounter{equation}{35}
|
\setcounter{equation}{35}
|
||||||
\setcounter{enumi}{4}
|
\setcounter{enumi}{4}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,85 +1,85 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {4}L'\IeC {\'e}nergie}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {7}L'\IeC {\'e}nergie}{97}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.1}Introduction}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.1}Introduction}{97}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.2}Travail}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.2}Travail}{97}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.1}{\ignorespaces Puissance}}{74}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.1}{\ignorespaces Puissance}}{98}\protected@file@percent }
|
||||||
\newlabel{chevalvapeur}{{4.1}{74}}
|
\newlabel{chevalvapeur}{{7.1}{98}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.3}Puissance}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.3}Puissance}{98}\protected@file@percent }
|
||||||
\newlabel{puissance}{{4.3}{74}}
|
\newlabel{puissance}{{7.3}{98}}
|
||||||
\newlabel{puiss}{{4.2}{74}}
|
\newlabel{puiss}{{7.2}{98}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.4}\IeC {\'E}nergie potentielle}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.4}\IeC {\'E}nergie potentielle}{98}\protected@file@percent }
|
||||||
\newlabel{defenpot}{{4.3}{74}}
|
\newlabel{defenpot}{{7.3}{98}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.5}\IeC {\'E}nergie cin\IeC {\'e}tique}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.5}\IeC {\'E}nergie cin\IeC {\'e}tique}{99}\protected@file@percent }
|
||||||
\newlabel{encindef}{{4.5}{75}}
|
\newlabel{encindef}{{7.5}{99}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.6}Th\IeC {\'e}or\IeC {\`e}me de l'\IeC {\'e}nergie cin\IeC {\'e}tique}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.6}Th\IeC {\'e}or\IeC {\`e}me de l'\IeC {\'e}nergie cin\IeC {\'e}tique}{99}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.7}Conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.7}Conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{99}\protected@file@percent }
|
||||||
\newlabel{enmecdef}{{4.7}{75}}
|
\newlabel{enmecdef}{{7.7}{99}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.2}{\ignorespaces \IeC {\'E}nergie cin\IeC {\'e}tique et potentielle}}{76}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.2}{\ignorespaces \IeC {\'E}nergie cin\IeC {\'e}tique et potentielle}}{100}\protected@file@percent }
|
||||||
\newlabel{encinpotcirc}{{4.2}{76}}
|
\newlabel{encinpotcirc}{{7.2}{100}}
|
||||||
\citation{LJ04}
|
\citation{LJ04}
|
||||||
\citation{HRaFL03}
|
\citation{HRaFL03}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.8}Variation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{77}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.8}Variation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{101}\protected@file@percent }
|
||||||
\newlabel{varenmec}{{4.8}{77}}
|
\newlabel{varenmec}{{7.8}{101}}
|
||||||
\newlabel{thmennoncons}{{4.8}{77}}
|
\newlabel{thmennoncons}{{7.8}{101}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.9}\IeC {\'E}nergies renouvelables}{77}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.9}\IeC {\'E}nergies renouvelables}{101}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.9.1}\IeC {\'E}nergie hydraulique}{77}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.9.1}\IeC {\'E}nergie hydraulique}{101}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.3}{\ignorespaces Barrage d'Emosson}}{78}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.3}{\ignorespaces Barrage d'Emosson}}{102}\protected@file@percent }
|
||||||
\newlabel{Emosson}{{4.3}{78}}
|
\newlabel{Emosson}{{7.3}{102}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Exemple}{78}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Exemple}{102}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Types de turbines}{79}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Types de turbines}{103}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.4}{\ignorespaces Turbine Pelton}}{79}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.4}{\ignorespaces Turbine Pelton}}{103}\protected@file@percent }
|
||||||
\newlabel{pelton}{{4.4}{79}}
|
\newlabel{pelton}{{7.4}{103}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.5}{\ignorespaces Ancienne turbine Pelton}}{79}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.5}{\ignorespaces Ancienne turbine Pelton}}{103}\protected@file@percent }
|
||||||
\newlabel{turbinepelton}{{4.5}{79}}
|
\newlabel{turbinepelton}{{7.5}{103}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Alternateur}{79}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Alternateur}{103}\protected@file@percent }
|
||||||
\citation{OP06}
|
\citation{OP06}
|
||||||
\citation{HRaFL03}
|
\citation{HRaFL03}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Probl\IeC {\`e}mes rencontr\IeC {\'e}s}{80}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Probl\IeC {\`e}mes rencontr\IeC {\'e}s}{104}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.9.2}\IeC {\'E}nergie \IeC {\'e}olienne}{80}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.9.2}\IeC {\'E}nergie \IeC {\'e}olienne}{104}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.6}{\ignorespaces \IeC {\'E}olienne}}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.6}{\ignorespaces \IeC {\'E}olienne}}{104}\protected@file@percent }
|
||||||
\newlabel{eolienne}{{4.6}{80}}
|
\newlabel{eolienne}{{7.6}{104}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.7}{\ignorespaces Pale d'\IeC {\'e}olienne}}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.7}{\ignorespaces Pale d'\IeC {\'e}olienne}}{104}\protected@file@percent }
|
||||||
\newlabel{aile}{{4.7}{80}}
|
\newlabel{aile}{{7.7}{104}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.8}{\ignorespaces Tube de vent\relax }}{81}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.8}{\ignorespaces Tube de vent\relax }}{105}\protected@file@percent }
|
||||||
\newlabel{tubecourant}{{4.8}{81}}
|
\newlabel{tubecourant}{{7.8}{105}}
|
||||||
\newlabel{puissvent}{{4.10}{81}}
|
\newlabel{puissvent}{{7.10}{105}}
|
||||||
\newlabel{puissdebetz}{{4.12}{81}}
|
\newlabel{puissdebetz}{{7.12}{105}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.9.3}\IeC {\'E}nergie solaire}{81}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.9.3}\IeC {\'E}nergie solaire}{105}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie solaire thermique}{81}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie solaire thermique}{105}\protected@file@percent }
|
||||||
\newlabel{puissincidphoto}{{4.13}{82}}
|
\newlabel{puissincidphoto}{{7.13}{106}}
|
||||||
\newlabel{puisssolthermique}{{4.14}{82}}
|
\newlabel{puisssolthermique}{{7.14}{106}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.9}{\ignorespaces Solaire thermique}}{83}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.9}{\ignorespaces Solaire thermique}}{107}\protected@file@percent }
|
||||||
\newlabel{solairethermique}{{4.9}{83}}
|
\newlabel{solairethermique}{{7.9}{107}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie solaire \IeC {\'e}lectrique}{83}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie solaire \IeC {\'e}lectrique}{107}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.10}{\ignorespaces Effet photo\IeC {\'e}lectrique}}{83}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.10}{\ignorespaces Effet photo\IeC {\'e}lectrique}}{107}\protected@file@percent }
|
||||||
\newlabel{effetphotoelectrique}{{4.10}{83}}
|
\newlabel{effetphotoelectrique}{{7.10}{107}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.11}{\ignorespaces Cellule photo\IeC {\'e}lectrique}}{84}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.11}{\ignorespaces Cellule photo\IeC {\'e}lectrique}}{108}\protected@file@percent }
|
||||||
\newlabel{cellulephotoelectrique}{{4.11}{84}}
|
\newlabel{cellulephotoelectrique}{{7.11}{108}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.9.4}\IeC {\'E}nergie g\IeC {\'e}othermique}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.9.4}\IeC {\'E}nergie g\IeC {\'e}othermique}{108}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.10}\IeC {\'E}nergies non renouvelables}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {7.10}\IeC {\'E}nergies non renouvelables}{108}\protected@file@percent }
|
||||||
\citation{HRaFL03}
|
\citation{HRaFL03}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.12}{\ignorespaces Applications de la g\IeC {\'e}othermie}}{85}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.12}{\ignorespaces Applications de la g\IeC {\'e}othermie}}{109}\protected@file@percent }
|
||||||
\newlabel{geothermieapplications}{{4.12}{85}}
|
\newlabel{geothermieapplications}{{7.12}{109}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.10.1}\IeC {\'E}nergie nucl\IeC {\'e}aire}{85}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.10.1}\IeC {\'E}nergie nucl\IeC {\'e}aire}{109}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Fission}{85}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Fission}{109}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.13}{\ignorespaces Fission de l'uranium\relax }}{86}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.13}{\ignorespaces Fission de l'uranium\relax }}{110}\protected@file@percent }
|
||||||
\newlabel{FissionUranium}{{4.13}{86}}
|
\newlabel{FissionUranium}{{7.13}{110}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}chets radioactifs}{86}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{D\IeC {\'e}chets radioactifs}{110}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.14}{\ignorespaces R\IeC {\'e}acteur nucl\IeC {\'e}aire\relax }}{86}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.14}{\ignorespaces R\IeC {\'e}acteur nucl\IeC {\'e}aire\relax }}{110}\protected@file@percent }
|
||||||
\newlabel{reacteurnucleaire}{{4.14}{86}}
|
\newlabel{reacteurnucleaire}{{7.14}{110}}
|
||||||
\citation{SV06}
|
\citation{SV06}
|
||||||
\citation{HRaFL03}
|
\citation{HRaFL03}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Accidents nucl\IeC {\'e}aires}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Accidents nucl\IeC {\'e}aires}{111}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Fusion}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Fusion}{111}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.10.2}\IeC {\'E}nergie de combustion~: p\IeC {\'e}trole et gaz}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {7.10.2}\IeC {\'E}nergie de combustion~: p\IeC {\'e}trole et gaz}{111}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.15}{\ignorespaces Combustion du m\IeC {\'e}thane}}{88}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.15}{\ignorespaces Combustion du m\IeC {\'e}thane}}{112}\protected@file@percent }
|
||||||
\newlabel{combustiongaz}{{4.15}{88}}
|
\newlabel{combustiongaz}{{7.15}{112}}
|
||||||
\newlabel{RF3}{89}
|
\newlabel{RF3}{113}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.16}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de l'\IeC {\'e}nergie\relax }}{89}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {7.16}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de l'\IeC {\'e}nergie\relax }}{113}\protected@file@percent }
|
||||||
\@setckpt{Energie/Energie}{
|
\@setckpt{Energie/Energie}{
|
||||||
\setcounter{page}{90}
|
\setcounter{page}{114}
|
||||||
\setcounter{equation}{26}
|
\setcounter{equation}{26}
|
||||||
\setcounter{enumi}{7}
|
\setcounter{enumi}{7}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
@ -88,7 +88,7 @@
|
|||||||
\setcounter{footnote}{1}
|
\setcounter{footnote}{1}
|
||||||
\setcounter{mpfootnote}{0}
|
\setcounter{mpfootnote}{0}
|
||||||
\setcounter{part}{0}
|
\setcounter{part}{0}
|
||||||
\setcounter{chapter}{4}
|
\setcounter{chapter}{7}
|
||||||
\setcounter{section}{10}
|
\setcounter{section}{10}
|
||||||
\setcounter{subsection}{2}
|
\setcounter{subsection}{2}
|
||||||
\setcounter{subsubsection}{0}
|
\setcounter{subsubsection}{0}
|
||||||
@ -109,7 +109,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{0}
|
\setcounter{caption@flags}{0}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{49}
|
\setcounter{endnote}{50}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,65 +1,65 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {8}L'\IeC {\'e}nergie}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {8}L'\IeC {\'e}nergie}{115}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.1}Introduction}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.1}Introduction}{115}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.1}{\ignorespaces \IeC {\'E}nergie et vitesse\relax }}{119}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.1}{\ignorespaces \IeC {\'E}nergie et vitesse\relax }}{115}\protected@file@percent }
|
||||||
\newlabel{energie}{{8.1}{119}}
|
\newlabel{energie}{{8.1}{115}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.2}Le travail}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.2}Le travail}{115}\protected@file@percent }
|
||||||
\newlabel{historiquement}{{8.2.1}{119}}
|
\newlabel{historiquement}{{8.2.1}{115}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.2.1}Historiquement}{119}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.2.1}Historiquement}{115}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.2}{\ignorespaces Balance \IeC {\`a} fl\IeC {\'e}au\relax }}{119}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.2}{\ignorespaces Balance \IeC {\`a} fl\IeC {\'e}au\relax }}{115}\protected@file@percent }
|
||||||
\newlabel{balance}{{8.2}{119}}
|
\newlabel{balance}{{8.2}{115}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.2.2}D\IeC {\'e}finition}{120}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.2.2}D\IeC {\'e}finition}{116}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Travail simple}{120}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Travail simple}{116}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.3}{\ignorespaces Travail simple\relax }}{120}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.3}{\ignorespaces Travail simple\relax }}{116}\protected@file@percent }
|
||||||
\newlabel{travailsimple}{{8.3}{120}}
|
\newlabel{travailsimple}{{8.3}{116}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Travail et produit scalaire}{120}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Travail et produit scalaire}{116}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.4}{\ignorespaces Travail et produit scalaire\relax }}{120}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.4}{\ignorespaces Travail et produit scalaire\relax }}{116}\protected@file@percent }
|
||||||
\newlabel{travailvecteur}{{8.4}{120}}
|
\newlabel{travailvecteur}{{8.4}{116}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Travail cas g\IeC {\'e}n\IeC {\'e}ral}{120}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Travail cas g\IeC {\'e}n\IeC {\'e}ral}{116}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.5}{\ignorespaces Travail en g\IeC {\'e}n\IeC {\'e}ral\relax }}{120}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.5}{\ignorespaces Travail en g\IeC {\'e}n\IeC {\'e}ral\relax }}{116}\protected@file@percent }
|
||||||
\newlabel{travailgeneral}{{8.5}{120}}
|
\newlabel{travailgeneral}{{8.5}{116}}
|
||||||
\newlabel{travail}{{8.1}{121}}
|
\newlabel{travail}{{8.1}{117}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.3}L'\IeC {\'e}nergie}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.3}L'\IeC {\'e}nergie}{117}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.1}Introduction}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.1}Introduction}{117}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.2}\IeC {\'E}nergie potentielle}{121}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.2}\IeC {\'E}nergie potentielle}{117}\protected@file@percent }
|
||||||
\newlabel{enpotdef}{{8.2}{122}}
|
\newlabel{enpotdef}{{8.2}{118}}
|
||||||
\newlabel{\IeC {\'e}nergie cin\IeC {\'e}tique}{{8.3.3}{122}}
|
\newlabel{\IeC {\'e}nergie cin\IeC {\'e}tique}{{8.3.3}{118}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{118}\protected@file@percent }
|
||||||
\newlabel{eqencindef}{{8.3}{122}}
|
\newlabel{eqencindef}{{8.3}{118}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.4}\IeC {\'E}nergie m\IeC {\'e}canique}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.4}\IeC {\'E}nergie m\IeC {\'e}canique}{118}\protected@file@percent }
|
||||||
\newlabel{enmec}{{8.4}{122}}
|
\newlabel{enmec}{{8.4}{118}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.5}Exemple}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.3.5}Exemple}{118}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.4}Conservation de l'\IeC {\'e}nergie}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.4}Conservation de l'\IeC {\'e}nergie}{118}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.1}Introduction}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.1}Introduction}{118}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.2}Th\IeC {\'e}or\IeC {\`e}me de conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{122}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.2}Th\IeC {\'e}or\IeC {\`e}me de conservation de l'\IeC {\'e}nergie m\IeC {\'e}canique}{118}\protected@file@percent }
|
||||||
\newlabel{consenmec0}{{8.5}{123}}
|
\newlabel{consenmec0}{{8.5}{119}}
|
||||||
\newlabel{consenmec}{{8.6}{123}}
|
\newlabel{consenmec}{{8.6}{119}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.3}Exemples}{123}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.4.3}Exemples}{119}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.5}Limite du th\IeC {\'e}or\IeC {\`e}me de conservation}{124}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.5}Limite du th\IeC {\'e}or\IeC {\`e}me de conservation}{120}\protected@file@percent }
|
||||||
\newlabel{mecnc}{{8.14}{124}}
|
\newlabel{mecnc}{{8.14}{120}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {8.6}Forces conservatives}{124}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {8.6}Forces conservatives}{120}\protected@file@percent }
|
||||||
\newlabel{conservatives}{{8.6}{124}}
|
\newlabel{conservatives}{{8.6}{120}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.1}D\IeC {\'e}finition}{124}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.1}D\IeC {\'e}finition}{120}\protected@file@percent }
|
||||||
\newlabel{forceconservative}{{8.15}{124}}
|
\newlabel{forceconservative}{{8.15}{120}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.2}Exemples}{124}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.2}Exemples}{120}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Le poids}{124}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Le poids}{120}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.6}{\ignorespaces Travail du poids\relax }}{125}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.6}{\ignorespaces Travail du poids\relax }}{121}\protected@file@percent }
|
||||||
\newlabel{travailferme}{{8.6}{125}}
|
\newlabel{travailferme}{{8.6}{121}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Le ressort}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Le ressort}{121}\protected@file@percent }
|
||||||
\newlabel{enpotres}{{8.16}{125}}
|
\newlabel{enpotres}{{8.16}{121}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.3}G\IeC {\'e}n\IeC {\'e}ralisation}{125}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {8.6.3}G\IeC {\'e}n\IeC {\'e}ralisation}{121}\protected@file@percent }
|
||||||
\newlabel{fderiveenpot}{{8.17}{126}}
|
\newlabel{fderiveenpot}{{8.17}{122}}
|
||||||
\newlabel{fintenpot}{{8.18}{126}}
|
\newlabel{fintenpot}{{8.18}{122}}
|
||||||
\newlabel{enpotvsf}{{8.19}{126}}
|
\newlabel{enpotvsf}{{8.19}{122}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie gravifique}{126}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}nergie gravifique}{122}\protected@file@percent }
|
||||||
\newlabel{forcedegravitation}{{8.20}{126}}
|
\newlabel{forcedegravitation}{{8.20}{122}}
|
||||||
\newlabel{enpotgrav}{{8.21}{126}}
|
\newlabel{enpotgrav}{{8.21}{122}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {8.7}{\ignorespaces Force et \IeC {\'e}nergie potentielle de gravitation entre la Terre et le Soleil\relax }}{127}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {8.7}{\ignorespaces Force et \IeC {\'e}nergie potentielle de gravitation entre la Terre et le Soleil\relax }}{123}\protected@file@percent }
|
||||||
\newlabel{forceetenpotST}{{8.7}{127}}
|
\newlabel{forceetenpotST}{{8.7}{123}}
|
||||||
\@setckpt{EnergieOS/EnergieOS}{
|
\@setckpt{EnergieOS/EnergieOS}{
|
||||||
\setcounter{page}{128}
|
\setcounter{page}{124}
|
||||||
\setcounter{equation}{21}
|
\setcounter{equation}{21}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,84 +1,84 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {1}Introduction}{21}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {1}Introduction}{17}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {1.1}Du temps}{21}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {1.1}Du temps}{17}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {1.2}De l'infiniment grand \IeC {\`a} l'infiniment petit}{21}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {1.2}De l'infiniment grand \IeC {\`a} l'infiniment petit}{17}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.1}L'Univers}{21}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.1}L'Univers}{17}\protected@file@percent }
|
||||||
\citation{JR00}
|
\citation{JR00}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.1}{\ignorespaces L'univers profond}}{22}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.1}{\ignorespaces L'univers profond}}{18}\protected@file@percent }
|
||||||
\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
|
\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
|
||||||
\newlabel{universprofond}{{1.1}{22}}
|
\newlabel{universprofond}{{1.1}{18}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.2}{\ignorespaces Mod\IeC {\`e}les de courbure}}{22}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.2}{\ignorespaces Mod\IeC {\`e}les de courbure}}{18}\protected@file@percent }
|
||||||
\newlabel{modeledecourbure}{{1.2}{22}}
|
\newlabel{modeledecourbure}{{1.2}{18}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.2}Les amas de galaxies}{22}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.2}Les amas de galaxies}{18}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.3}{\ignorespaces L'\IeC {\'e}volution du Soleil}}{23}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.3}{\ignorespaces L'\IeC {\'e}volution du Soleil}}{19}\protected@file@percent }
|
||||||
\newlabel{evosol}{{1.3}{23}}
|
\newlabel{evosol}{{1.3}{19}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.3}Les galaxies}{23}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.3}Les galaxies}{19}\protected@file@percent }
|
||||||
\citation{FC05}
|
\citation{FC05}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.4}{\ignorespaces Groupe local}}{24}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.4}{\ignorespaces Groupe local}}{20}\protected@file@percent }
|
||||||
\newlabel{localesgalaxies}{{1.4}{24}}
|
\newlabel{localesgalaxies}{{1.4}{20}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.5}{\ignorespaces Galaxie du Sombrero}}{24}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.5}{\ignorespaces Galaxie du Sombrero}}{20}\protected@file@percent }
|
||||||
\newlabel{galaxies}{{1.5}{24}}
|
\newlabel{galaxies}{{1.5}{20}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.4}Les \IeC {\'e}toiles}{24}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.4}Les \IeC {\'e}toiles}{20}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.5}Le syst\IeC {\`e}me solaire}{24}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.5}Le syst\IeC {\`e}me solaire}{20}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.6}{\ignorespaces Interaction de deux galaxies}}{25}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.6}{\ignorespaces Interaction de deux galaxies}}{21}\protected@file@percent }
|
||||||
\newlabel{choc}{{1.6}{25}}
|
\newlabel{choc}{{1.6}{21}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.7}{\ignorespaces N\IeC {\'e}buleuse plan\IeC {\'e}taire}}{25}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.7}{\ignorespaces N\IeC {\'e}buleuse plan\IeC {\'e}taire}}{21}\protected@file@percent }
|
||||||
\newlabel{planetaire}{{1.7}{25}}
|
\newlabel{planetaire}{{1.7}{21}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.8}{\ignorespaces Premi\IeC {\`e}re exoplan\IeC {\`e}te}}{25}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.8}{\ignorespaces Premi\IeC {\`e}re exoplan\IeC {\`e}te}}{21}\protected@file@percent }
|
||||||
\newlabel{2M1207}{{1.8}{25}}
|
\newlabel{2M1207}{{1.8}{21}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.6}La Terre et la Lune}{26}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.6}La Terre et la Lune}{22}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{La Terre}{26}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{La Terre}{22}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.9}{\ignorespaces Syst\IeC {\`e}me solaire}}{27}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.9}{\ignorespaces Syst\IeC {\`e}me solaire}}{23}\protected@file@percent }
|
||||||
\newlabel{systemesolaire}{{1.9}{27}}
|
\newlabel{systemesolaire}{{1.9}{23}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{La Lune}{27}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{La Lune}{23}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.10}{\ignorespaces La taille des plan\IeC {\`e}tes}}{28}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.10}{\ignorespaces La taille des plan\IeC {\`e}tes}}{24}\protected@file@percent }
|
||||||
\newlabel{lesplanetes}{{1.10}{28}}
|
\newlabel{lesplanetes}{{1.10}{24}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.11}{\ignorespaces La taille des plan\IeC {\`e}tes}}{29}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.11}{\ignorespaces La taille des plan\IeC {\`e}tes}}{25}\protected@file@percent }
|
||||||
\newlabel{billetcomete}{{1.11}{29}}
|
\newlabel{billetcomete}{{1.11}{25}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.12}{\ignorespaces Une com\IeC {\`e}te}}{29}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.12}{\ignorespaces Une com\IeC {\`e}te}}{25}\protected@file@percent }
|
||||||
\newlabel{comete}{{1.12}{29}}
|
\newlabel{comete}{{1.12}{25}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.13}{\ignorespaces \IeC {\'E}toiles filantes}}{29}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.13}{\ignorespaces \IeC {\'E}toiles filantes}}{25}\protected@file@percent }
|
||||||
\newlabel{Leonides}{{1.13}{29}}
|
\newlabel{Leonides}{{1.13}{25}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Les mar\IeC {\'e}es}{29}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Les mar\IeC {\'e}es}{25}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.14}{\ignorespaces Les saisons}}{30}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.14}{\ignorespaces Les saisons}}{26}\protected@file@percent }
|
||||||
\newlabel{saisonsperso}{{1.14}{30}}
|
\newlabel{saisonsperso}{{1.14}{26}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.15}{\ignorespaces Les saisons}}{30}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.15}{\ignorespaces Les saisons}}{26}\protected@file@percent }
|
||||||
\newlabel{pointingsaisons}{{1.15}{30}}
|
\newlabel{pointingsaisons}{{1.15}{26}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.16}{\ignorespaces La terre et la lune}}{30}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.16}{\ignorespaces La terre et la lune}}{26}\protected@file@percent }
|
||||||
\newlabel{terrelune}{{1.16}{30}}
|
\newlabel{terrelune}{{1.16}{26}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.17}{\ignorespaces Les phases de la lune}}{31}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.17}{\ignorespaces Les phases de la lune}}{27}\protected@file@percent }
|
||||||
\newlabel{phasesdelalune}{{1.17}{31}}
|
\newlabel{phasesdelalune}{{1.17}{27}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.18}{\ignorespaces Orbites de la lune et du soleil}}{31}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.18}{\ignorespaces Orbites de la lune et du soleil}}{27}\protected@file@percent }
|
||||||
\newlabel{Orbite-lune-soleil}{{1.18}{31}}
|
\newlabel{Orbite-lune-soleil}{{1.18}{27}}
|
||||||
\citation{SV06}
|
\citation{SV06}
|
||||||
\citation{FB05}
|
\citation{FB05}
|
||||||
\newlabel{marees2}{{1.19(a)}{32}}
|
\newlabel{marees2}{{1.19(a)}{28}}
|
||||||
\newlabel{sub@marees2}{{(a)}{32}}
|
\newlabel{sub@marees2}{{(a)}{28}}
|
||||||
\newlabel{marees1}{{1.19(b)}{32}}
|
\newlabel{marees1}{{1.19(b)}{28}}
|
||||||
\newlabel{sub@marees1}{{(b)}{32}}
|
\newlabel{sub@marees1}{{(b)}{28}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.19}{\ignorespaces Les mar\IeC {\'e}es\relax }}{32}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.19}{\ignorespaces Les mar\IeC {\'e}es\relax }}{28}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Sans rotation de la lune}}}{32}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Sans rotation de la lune}}}{28}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Avec rotation de la lune}}}{32}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Avec rotation de la lune}}}{28}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.7}Le monde subatomique}{32}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {1.2.7}Le monde subatomique}{28}\protected@file@percent }
|
||||||
\newlabel{subsectionsubatomique}{{1.2.7}{32}}
|
\newlabel{subsectionsubatomique}{{1.2.7}{28}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.20}{\ignorespaces La n\IeC {\'e}buleuse du Crabe}}{32}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.20}{\ignorespaces La n\IeC {\'e}buleuse du Crabe}}{28}\protected@file@percent }
|
||||||
\newlabel{crabnebula}{{1.20}{32}}
|
\newlabel{crabnebula}{{1.20}{28}}
|
||||||
\citation{SV06}
|
\citation{SV06}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.21}{\ignorespaces L'atome de Bohr}}{33}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.21}{\ignorespaces L'atome de Bohr}}{29}\protected@file@percent }
|
||||||
\newlabel{Bohr}{{1.21}{33}}
|
\newlabel{Bohr}{{1.21}{29}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {1.1}{\ignorespaces Tableau des particules \IeC {\'e}l\IeC {\'e}mentaires}}{34}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {1.1}{\ignorespaces Tableau des particules \IeC {\'e}l\IeC {\'e}mentaires}}{30}\protected@file@percent }
|
||||||
\newlabel{particuleselementaires}{{1.1}{34}}
|
\newlabel{particuleselementaires}{{1.1}{30}}
|
||||||
\citation{JL06}
|
\citation{JL06}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.22}{\ignorespaces L'atome~: onde de probabilit\IeC {\'e}}}{35}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.22}{\ignorespaces L'atome~: onde de probabilit\IeC {\'e}}}{31}\protected@file@percent }
|
||||||
\newlabel{ondeproba}{{1.22}{35}}
|
\newlabel{ondeproba}{{1.22}{31}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {1.23}{\ignorespaces L'orbitale~: onde de probabilit\IeC {\'e}}}{35}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {1.23}{\ignorespaces L'orbitale~: onde de probabilit\IeC {\'e}}}{31}\protected@file@percent }
|
||||||
\newlabel{orbitale}{{1.23}{35}}
|
\newlabel{orbitale}{{1.23}{31}}
|
||||||
\newlabel{forcefaible}{{1.2.7}{35}}
|
\newlabel{forcefaible}{{1.2.7}{31}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Conclusion}{36}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Conclusion}{32}\protected@file@percent }
|
||||||
\@setckpt{Introduction/Introduction}{
|
\@setckpt{Introduction/Introduction}{
|
||||||
\setcounter{page}{37}
|
\setcounter{page}{33}
|
||||||
\setcounter{equation}{0}
|
\setcounter{equation}{0}
|
||||||
\setcounter{enumi}{0}
|
\setcounter{enumi}{0}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,42 +1,42 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {5}M\IeC {\'e}canique diff\IeC {\'e}rentielle}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {5}M\IeC {\'e}canique diff\IeC {\'e}rentielle}{83}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.1}Introduction}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {5.1}Introduction}{83}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.2}Cin\IeC {\'e}matique}{87}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {5.2}Cin\IeC {\'e}matique}{83}\protected@file@percent }
|
||||||
\newlabel{cinemadiff}{{5.2}{87}}
|
\newlabel{cinemadiff}{{5.2}{83}}
|
||||||
\newlabel{posvitaccdiff}{{5.4}{87}}
|
\newlabel{posvitaccdiff}{{5.4}{83}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.1}Exemples}{88}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.1}Exemples}{84}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e}~: MRUA}{88}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Mouvement rectiligne uniform\IeC {\'e}ment acc\IeC {\'e}l\IeC {\'e}r\IeC {\'e}~: MRUA}{84}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Port\IeC {\'e} maximum en balistique}{88}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Port\IeC {\'e} maximum en balistique}{84}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.3}Dynamique}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {5.3}Dynamique}{85}\protected@file@percent }
|
||||||
\newlabel{diffma}{{5.7}{89}}
|
\newlabel{diffma}{{5.7}{85}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.3.1}Int\IeC {\'e}gration}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {5.3.1}Int\IeC {\'e}gration}{85}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Chute libre}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Chute libre}{85}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Freinage}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Freinage}{85}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.3.2}\IeC {\'E}quation diff\IeC {\'e}rentielle}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {5.3.2}\IeC {\'E}quation diff\IeC {\'e}rentielle}{85}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Chute dans un fluide visqueux}{89}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Chute dans un fluide visqueux}{85}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.1}{\ignorespaces Chute visqueuse\relax }}{90}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {5.1}{\ignorespaces Chute visqueuse\relax }}{86}\protected@file@percent }
|
||||||
\newlabel{chutevisqueuse}{{5.1}{90}}
|
\newlabel{chutevisqueuse}{{5.1}{86}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.2}{\ignorespaces Chute dans un fluide visqueux\relax }}{91}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {5.2}{\ignorespaces Chute dans un fluide visqueux\relax }}{87}\protected@file@percent }
|
||||||
\newlabel{figchutevisqueuse}{{5.2}{91}}
|
\newlabel{figchutevisqueuse}{{5.2}{87}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Mouvement harmonique}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Mouvement harmonique}{87}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.3}{\ignorespaces Masse oscillante\relax }}{91}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {5.3}{\ignorespaces Masse oscillante\relax }}{87}\protected@file@percent }
|
||||||
\newlabel{masseoscillante}{{5.3}{91}}
|
\newlabel{masseoscillante}{{5.3}{87}}
|
||||||
\newlabel{cond_init}{{5.8}{91}}
|
\newlabel{cond_init}{{5.8}{87}}
|
||||||
\newlabel{ressortposition}{{5.9}{91}}
|
\newlabel{ressortposition}{{5.9}{87}}
|
||||||
\newlabel{ressortvitesse}{{5.10}{91}}
|
\newlabel{ressortvitesse}{{5.10}{87}}
|
||||||
\newlabel{ressort1ersol}{{5.11}{92}}
|
\newlabel{ressort1ersol}{{5.11}{88}}
|
||||||
\newlabel{ressortvitmax}{{5.12}{92}}
|
\newlabel{ressortvitmax}{{5.12}{88}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Mouvement harmonique d'une masse pendante}{92}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Mouvement harmonique d'une masse pendante}{88}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.4}{\ignorespaces Masse suspendue\relax }}{92}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {5.4}{\ignorespaces Masse suspendue\relax }}{88}\protected@file@percent }
|
||||||
\newlabel{massesuspendue}{{5.4}{92}}
|
\newlabel{massesuspendue}{{5.4}{88}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.5}{\ignorespaces Masse oscillante suspendue\relax }}{93}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {5.5}{\ignorespaces Masse oscillante suspendue\relax }}{89}\protected@file@percent }
|
||||||
\newlabel{masseoscillantesuspendue}{{5.5}{93}}
|
\newlabel{masseoscillantesuspendue}{{5.5}{89}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Mouvement non lin\IeC {\'e}aire}{93}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Mouvement non lin\IeC {\'e}aire}{89}\protected@file@percent }
|
||||||
\newlabel{non-lineaire}{{5.14}{93}}
|
\newlabel{non-lineaire}{{5.14}{89}}
|
||||||
\@setckpt{MecaniqueDifferentielle/MecaniqueDifferentielle}{
|
\@setckpt{MecaniqueDifferentielle/MecaniqueDifferentielle}{
|
||||||
\setcounter{page}{94}
|
\setcounter{page}{90}
|
||||||
\setcounter{equation}{14}
|
\setcounter{equation}{14}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,77 +1,77 @@
|
|||||||
\relax
|
\relax
|
||||||
\newlabel{Mvt2dim}{{4}{73}}
|
\newlabel{Mvt2dim}{{4}{69}}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {4}M\IeC {\'e}canique en plusieurs dimensions}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {4}M\IeC {\'e}canique en plusieurs dimensions}{69}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.1}Pr\IeC {\'e}liminaires}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {4.1}Pr\IeC {\'e}liminaires}{69}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.1.1}Dimensions}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.1.1}Dimensions}{69}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.1.2}Syst\IeC {\`e}me d'axes}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.1.2}Syst\IeC {\`e}me d'axes}{69}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.2}Notion de vecteur en physique}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {4.2}Notion de vecteur en physique}{69}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.2.1}Norme d'un vecteur}{73}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.2.1}Norme d'un vecteur}{69}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.2.2}Op\IeC {\'e}rations vectorielles}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.2.2}Op\IeC {\'e}rations vectorielles}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{produit scalaire}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{produit scalaire}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Produit vectoriel}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Produit vectoriel}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.3}M\IeC {\'e}canique}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {4.3}M\IeC {\'e}canique}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.3.1}Cin\IeC {\'e}matique}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.3.1}Cin\IeC {\'e}matique}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Position}{74}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Position}{70}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Vitesse}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Vitesse}{71}\protected@file@percent }
|
||||||
\newlabel{vitinstant}{{4.2}{75}}
|
\newlabel{vitinstant}{{4.2}{71}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Acc\IeC {\'e}l\IeC {\'e}ration}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Acc\IeC {\'e}l\IeC {\'e}ration}{71}\protected@file@percent }
|
||||||
\newlabel{accinstant}{{4.4}{75}}
|
\newlabel{accinstant}{{4.4}{71}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.3.2}Dynamique}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.3.2}Dynamique}{71}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Premi\IeC {\`e}re loi}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Premi\IeC {\`e}re loi}{71}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.1}{\ignorespaces \IeC {\'E}quilibre statique\relax }}{75}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.1}{\ignorespaces \IeC {\'E}quilibre statique\relax }}{71}\protected@file@percent }
|
||||||
\newlabel{ballon}{{4.1}{75}}
|
\newlabel{ballon}{{4.1}{71}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Seconde loi}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Seconde loi}{71}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Troisi\IeC {\`e}me loi}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Troisi\IeC {\`e}me loi}{71}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {4.4}Exemples}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {4.4}Exemples}{71}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.1}Statique}{75}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.1}Statique}{71}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.2}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{76}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.2}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{72}\protected@file@percent }
|
||||||
\newlabel{planincline}{{4.2}{76}}
|
\newlabel{planincline}{{4.2}{72}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.2}Plan inclin\IeC {\'e}}{76}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.2}Plan inclin\IeC {\'e}}{72}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.3}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{77}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.3}{\ignorespaces Le plan inclin\IeC {\'e}\relax }}{73}\protected@file@percent }
|
||||||
\newlabel{planincline2}{{4.3}{77}}
|
\newlabel{planincline2}{{4.3}{73}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.4}{\ignorespaces Tir balistique\relax }}{78}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.4}{\ignorespaces Tir balistique\relax }}{74}\protected@file@percent }
|
||||||
\newlabel{tirbalistique}{{4.4}{78}}
|
\newlabel{tirbalistique}{{4.4}{74}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.3}Balistique}{78}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.3}Balistique}{74}\protected@file@percent }
|
||||||
\newlabel{Port\IeC {\'e}e}{{4.8}{79}}
|
\newlabel{Port\IeC {\'e}e}{{4.8}{75}}
|
||||||
\newlabel{deuxangles}{{4.5(a)}{80}}
|
\newlabel{deuxangles}{{4.5(a)}{76}}
|
||||||
\newlabel{sub@deuxangles}{{(a)}{80}}
|
\newlabel{sub@deuxangles}{{(a)}{76}}
|
||||||
\newlabel{unangle}{{4.5(b)}{80}}
|
\newlabel{unangle}{{4.5(b)}{76}}
|
||||||
\newlabel{sub@unangle}{{(b)}{80}}
|
\newlabel{sub@unangle}{{(b)}{76}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.5}{\ignorespaces Tirs balistiques\relax }}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.5}{\ignorespaces Tirs balistiques\relax }}{76}\protected@file@percent }
|
||||||
\newlabel{tir}{{4.5}{80}}
|
\newlabel{tir}{{4.5}{76}}
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Deux angles}}}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Deux angles}}}{76}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Un angle}}}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Un angle}}}{76}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.6}{\ignorespaces Parabole de s\IeC {\'e}curit\IeC {\'e}\relax }}{80}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.6}{\ignorespaces Parabole de s\IeC {\'e}curit\IeC {\'e}\relax }}{76}\protected@file@percent }
|
||||||
\newlabel{parabolesecurite}{{4.6}{80}}
|
\newlabel{parabolesecurite}{{4.6}{76}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.4}Mouvement circulaire uniforme~: MCU}{80}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.4}Mouvement circulaire uniforme~: MCU}{76}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{80}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{D\IeC {\'e}finition}{76}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Cin\IeC {\'e}matique}{80}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Cin\IeC {\'e}matique}{76}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Relation importante}{81}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Relation importante}{77}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.7}{\ignorespaces Mouvement circulaire uniforme\relax }}{81}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.7}{\ignorespaces Mouvement circulaire uniforme\relax }}{77}\protected@file@percent }
|
||||||
\newlabel{dimMCU}{{4.7}{81}}
|
\newlabel{dimMCU}{{4.7}{77}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Dynamique}{81}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Dynamique}{77}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Virages inclin\IeC {\'e}s}{81}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Virages inclin\IeC {\'e}s}{77}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Vitesses minimales}{82}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Vitesses minimales}{78}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.8}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse minimale\relax }}{82}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.8}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse minimale\relax }}{78}\protected@file@percent }
|
||||||
\newlabel{viragesvmin0}{{4.8}{82}}
|
\newlabel{viragesvmin0}{{4.8}{78}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.9}{\ignorespaces Virages inclin\IeC {\'e}~: vitesses minimale\relax }}{82}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.9}{\ignorespaces Virages inclin\IeC {\'e}~: vitesses minimale\relax }}{78}\protected@file@percent }
|
||||||
\newlabel{viragesvminpas0}{{4.9}{82}}
|
\newlabel{viragesvminpas0}{{4.9}{78}}
|
||||||
\@writefile{toc}{\contentsline {paragraph}{Vitesses maximales}{83}\protected@file@percent }
|
\@writefile{toc}{\contentsline {paragraph}{Vitesses maximales}{79}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {4.10}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse maximale\relax }}{83}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {4.10}{\ignorespaces Virages inclin\IeC {\'e}~: vitesse maximale\relax }}{79}\protected@file@percent }
|
||||||
\newlabel{viragesvmaxfinie}{{4.10}{83}}
|
\newlabel{viragesvmaxfinie}{{4.10}{79}}
|
||||||
\citation{GC88}
|
\citation{GC88}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.5}Satellite en orbite g\IeC {\'e}ostationnaire}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.5}Satellite en orbite g\IeC {\'e}ostationnaire}{80}\protected@file@percent }
|
||||||
\newlabel{dimgeostat}{{4.4.5}{84}}
|
\newlabel{dimgeostat}{{4.4.5}{80}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Introduction}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Introduction}{80}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Th\IeC {\'e}oriquement}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Th\IeC {\'e}oriquement}{80}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Num\IeC {\'e}riquement}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Num\IeC {\'e}riquement}{80}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.6}Mouvement central}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {4.4.6}Mouvement central}{80}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Mouvement kepleriens}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Mouvement kepleriens}{80}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Loi de Kepler}{84}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Loi de Kepler}{80}\protected@file@percent }
|
||||||
\@setckpt{MecaniqueDim/MecaniqueDim}{
|
\@setckpt{MecaniqueDim/MecaniqueDim}{
|
||||||
\setcounter{page}{86}
|
\setcounter{page}{82}
|
||||||
\setcounter{equation}{9}
|
\setcounter{equation}{9}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -1,27 +1,27 @@
|
|||||||
\relax
|
\relax
|
||||||
\citation{SU03}
|
\citation{SU03}
|
||||||
\citation{SU03}
|
\citation{SU03}
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {9}Physique th\IeC {\'e}orique}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {9}Physique th\IeC {\'e}orique}{125}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{physiquetheorique}{{9}{129}}
|
\newlabel{physiquetheorique}{{9}{125}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.1}Introduction}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.1}Introduction}{125}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.2}\IeC {\'E}nergie potentielle}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.2}\IeC {\'E}nergie potentielle}{125}\protected@file@percent }
|
||||||
\newlabel{thfderiveenpot}{{9.1}{129}}
|
\newlabel{thfderiveenpot}{{9.1}{125}}
|
||||||
\newlabel{thfintenpot}{{9.2}{129}}
|
\newlabel{thfintenpot}{{9.2}{125}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{125}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.4}Quantit\IeC {\'e} de mouvement}{129}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.4}Quantit\IeC {\'e} de mouvement}{125}\protected@file@percent }
|
||||||
\newlabel{thconsqtitemvt}{{9.4}{129}}
|
\newlabel{thconsqtitemvt}{{9.4}{125}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.5}Conservation de l'\IeC {\'e}nergie}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.5}Conservation de l'\IeC {\'e}nergie}{126}\protected@file@percent }
|
||||||
\newlabel{thconsenmec0}{{9.5}{130}}
|
\newlabel{thconsenmec0}{{9.5}{126}}
|
||||||
\newlabel{thenmec}{{9.6}{130}}
|
\newlabel{thenmec}{{9.6}{126}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.6}Principe de moindre action}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.6}Principe de moindre action}{126}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.1}Lagrangien}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.1}Lagrangien}{126}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.2}Action}{130}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.2}Action}{126}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.3}Minimalisation}{131}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {9.6.3}Minimalisation}{127}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {9.7}Euler-Lagrange}{131}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {9.7}Euler-Lagrange}{127}\protected@file@percent }
|
||||||
\@setckpt{PhysiqueTheorique/PhysiqueTheorique}{
|
\@setckpt{PhysiqueTheorique/PhysiqueTheorique}{
|
||||||
\setcounter{page}{133}
|
\setcounter{page}{129}
|
||||||
\setcounter{equation}{10}
|
\setcounter{equation}{10}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
@ -30,9 +30,13 @@
|
|||||||
\medskip
|
\medskip
|
||||||
Ce cours de mécanique et énergie a été écrit au début avec le logiciel de PAO Lyx, une interface graphique au célèbre Latex et aujourd'hui directement en latex. Il a donc été créé dans un environnement (ces deux logiciels tournant sous GNU-Linux) libre dont l'objectif est de contribuer au progrès en mettant à disposition de chacun, pour un coût moindre, le travail de milliers de programmeurs bénévoles. Dans ce cadre, il était naturel de permettre à chaque étudiant d'avoir accès à ce cours librement. C'est pourquoi, à l'instar des logiciels, il est distribué sous licence GFDL, licence de documentation libre. Attention cependant aux images qui ne sont pas toutes sous licence GFDL, mais peuvent être soumises à une autre licence libre ou être dans le domaine publique. Cela peut avoir une importance dans certains cas.
|
Ce cours de mécanique et énergie a été écrit au début avec le logiciel de PAO Lyx, une interface graphique au célèbre Latex et aujourd'hui directement en latex. Il a donc été créé dans un environnement (ces deux logiciels tournant sous GNU-Linux) libre dont l'objectif est de contribuer au progrès en mettant à disposition de chacun, pour un coût moindre, le travail de milliers de programmeurs bénévoles. Dans ce cadre, il était naturel de permettre à chaque étudiant d'avoir accès à ce cours librement. C'est pourquoi, à l'instar des logiciels, il est distribué sous licence GFDL, licence de documentation libre. Attention cependant aux images qui ne sont pas toutes sous licence GFDL, mais peuvent être soumises à une autre licence libre ou être dans le domaine publique. Cela peut avoir une importance dans certains cas.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Ce cours est aussi disponible sous licence Creative Commons CC-By-Sa 4 et ultérieure.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
Normalement la licence GFDL\index{licence@licence!GFDL} doit figurer avec le cours. Ce n'est pas le cas et ce pour ne pas allonger trop le texte. Mais le texte de la GFDL se trouve partout sur internet et il suffit d'un moteur de recherche pour le trouver. Par ailleurs, le texte de ce cours et ses sources \LaTeX sont disponibles en téléchargement à l'adresse
|
Normalement la licence GFDL\index{licence@licence!GFDL} doit figurer avec le cours. Ce n'est pas le cas et ce pour ne pas allonger trop le texte. Mais le texte de la GFDL se trouve partout sur internet et il suffit d'un moteur de recherche pour le trouver. Par ailleurs, le texte de ce cours et ses sources \LaTeX sont disponibles en téléchargement à l'adresse
|
||||||
|
|
||||||
\begin{center}https://framagit.org/users/guyotv/projects\end{center}
|
\begin{center}https://git.roflcopter.fr/users/guyotv/projects\end{center}
|
||||||
|
|
||||||
Pour tout renseignement complémentaire s'adresser à~:
|
Pour tout renseignement complémentaire s'adresser à~:
|
||||||
|
|
||||||
|
|||||||
@ -1,39 +1,39 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {6}Quantit\IeC {\'e} de mouvement}{95}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {6}Quantit\IeC {\'e} de mouvement}{91}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.1}Introduction}{95}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.1}Introduction}{91}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.2}Quantit\IeC {\'e} de mouvement}{95}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.2}Quantit\IeC {\'e} de mouvement}{91}\protected@file@percent }
|
||||||
\newlabel{3eloichoc}{{6.1}{95}}
|
\newlabel{3eloichoc}{{6.1}{91}}
|
||||||
\newlabel{2sur1}{{6.2}{95}}
|
\newlabel{2sur1}{{6.2}{91}}
|
||||||
\newlabel{1sur2}{{6.3}{95}}
|
\newlabel{1sur2}{{6.3}{91}}
|
||||||
\newlabel{achoc}{{6.4}{95}}
|
\newlabel{achoc}{{6.4}{91}}
|
||||||
\newlabel{varqtitedemvt}{{6.5}{95}}
|
\newlabel{varqtitedemvt}{{6.5}{91}}
|
||||||
\newlabel{qtitedemvt}{{6.6}{95}}
|
\newlabel{qtitedemvt}{{6.6}{91}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {6.2.1}Masse d'inertie}{95}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {6.2.1}Masse d'inertie}{91}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{96}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.3}\IeC {\'E}nergie cin\IeC {\'e}tique}{92}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.4}Choc parfaitement \IeC {\'e}lastique}{96}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.4}Choc parfaitement \IeC {\'e}lastique}{92}\protected@file@percent }
|
||||||
\newlabel{qtitemvt1dim}{{6.8}{96}}
|
\newlabel{qtitemvt1dim}{{6.8}{92}}
|
||||||
\newlabel{encin1dim}{{6.9}{96}}
|
\newlabel{encin1dim}{{6.9}{92}}
|
||||||
\newlabel{qtitemvtsuppr}{{6.10}{96}}
|
\newlabel{qtitemvtsuppr}{{6.10}{92}}
|
||||||
\newlabel{encincarre}{{6.11}{96}}
|
\newlabel{encincarre}{{6.11}{92}}
|
||||||
\newlabel{encinremarquable}{{6.12}{96}}
|
\newlabel{encinremarquable}{{6.12}{92}}
|
||||||
\newlabel{qtitemvtvitrelative}{{6.13}{96}}
|
\newlabel{qtitemvtvitrelative}{{6.13}{92}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {6.4.1}Exemple}{96}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {6.4.1}Exemple}{92}\protected@file@percent }
|
||||||
\newlabel{chocsimplemvt}{{6.14}{97}}
|
\newlabel{chocsimplemvt}{{6.14}{93}}
|
||||||
\newlabel{chocsimpleen}{{6.15}{97}}
|
\newlabel{chocsimpleen}{{6.15}{93}}
|
||||||
\newlabel{solv1'}{{6.16}{97}}
|
\newlabel{solv1'}{{6.16}{93}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.5}Choc parfaitement mou}{97}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.5}Choc parfaitement mou}{93}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {6.5.1}Exemple}{97}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {6.5.1}Exemple}{93}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.6}choc bidimentionnel}{98}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.6}choc bidimentionnel}{94}\protected@file@percent }
|
||||||
\newlabel{consqtitemvt}{{6.17}{98}}
|
\newlabel{consqtitemvt}{{6.17}{94}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {6.6.1}Exemple}{98}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {6.6.1}Exemple}{94}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {6.1}{\ignorespaces Choc 2 dim}}{99}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {6.1}{\ignorespaces Choc 2 dim}}{95}\protected@file@percent }
|
||||||
\newlabel{choc2dimimpact}{{6.1}{99}}
|
\newlabel{choc2dimimpact}{{6.1}{95}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {6.7}Impulsion}{99}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {6.7}Impulsion}{95}\protected@file@percent }
|
||||||
\newlabel{qtitemvtimpuls}{{6.7}{99}}
|
\newlabel{qtitemvtimpuls}{{6.7}{95}}
|
||||||
\@setckpt{QtiteMvt/QtiteMvt}{
|
\@setckpt{QtiteMvt/QtiteMvt}{
|
||||||
\setcounter{page}{100}
|
\setcounter{page}{96}
|
||||||
\setcounter{equation}{18}
|
\setcounter{equation}{18}
|
||||||
\setcounter{enumi}{2}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
616
SolutionsOS.tex
616
SolutionsOS.tex
@ -0,0 +1,616 @@
|
|||||||
|
\begin{Solution OS}{1}
|
||||||
|
La masse m constitue évidemment le système. On choisit un système d'axes vertical et horizontal dirigé vers le haut et dans le sens de l'accélération.
|
||||||
|
|
||||||
|
Les forces extérieures exercées sur la masse sont au nombre de trois~: son poids P, la réaction du plan R et la force F.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\caption[Force inclinée]{Une force inclinée}\label{forceinclinee}
|
||||||
|
\smallskip
|
||||||
|
\begin{center}
|
||||||
|
\def\svgwidth{6cm}
|
||||||
|
\input{Annexe-Exercices/Images/forceinclinee.eps_tex}
|
||||||
|
\end{center}
|
||||||
|
\end{figure}
|
||||||
|
La figure \ref{forceinclinee} présente la situation. On peut y voir les trois forces extérieures et, en rouge , la décomposition de la force F en ses composantes sur les axes (remarquez qu'on a représenté les composantes par des vecteurs, ce qui est courant en physique lors de la décomposition de forces parce qu'on peut alors comprendre celle-ci comme un remplacement de la force F par deux forces qui en forment la somme).
|
||||||
|
|
||||||
|
L'équation de Newton sous forme vectorielle donne alors les équations du mouvement en composantes~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum \overrightarrow{F}^{ext}=\overrightarrow{R}+\overrightarrow{P}+\overrightarrow{F}&=m\cdot \overrightarrow{a}\;\Rightarrow\\[0.8em]
|
||||||
|
F_x&=m\cdot a\\
|
||||||
|
R-P-F_y&=0
|
||||||
|
\end{align*}
|
||||||
|
car l'accélération selon l'axe y est nulle puisque la masse ne se déplace par sur cet axe.
|
||||||
|
|
||||||
|
En considérant le triangle formé par la force F, sa composante sur l'axe x et l'angle \(\alpha\), on peut écrire~:
|
||||||
|
\[F_x=F\cdot \cos(\alpha)\;\;\text{et}\;\;F_y=F\cdot \sin(\alpha)\]
|
||||||
|
et à l'aide de la définition du poids (\(P=m\cdot g\)), préciser les équations du mouvement~:
|
||||||
|
\begin{align*}
|
||||||
|
F\cdot \cos(\alpha)&=m\cdot a\\
|
||||||
|
R-m\cdot g-F\cdot \sin(\alpha)&=0
|
||||||
|
\end{align*}
|
||||||
|
Cela permet finalement les résultats~:
|
||||||
|
\begin{align*}
|
||||||
|
a&=\frac{F\cdot \cos(\alpha)}{m}\\
|
||||||
|
&=\frac{5\cdot \cos(30)}{15}=\SI{0,29}{\metre\per\second\squared}\\
|
||||||
|
R&=m\cdot g+F\cdot \sin(\alpha)\\
|
||||||
|
&=15\cdot 9.81+5\cdot \sin(30)=\SI{149,65}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{2}
|
||||||
|
Commençons par trouver les forces exercées par les câbles sur la lampe. Considérons donc la lampe comme système. Pour des câbles souples la force est exercée le long du câble. La situation est donc celle de la figure \ref{lampe}.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\caption[Lampe suspendue]{Une lampe suspendue}\label{lampe}
|
||||||
|
\smallskip
|
||||||
|
\begin{center}
|
||||||
|
\def\svgwidth{6cm}
|
||||||
|
\input{Annexe-Exercices/Images/lampe.eps_tex}
|
||||||
|
\end{center}
|
||||||
|
\end{figure}
|
||||||
|
Où R et F sont les tension dans les câbles. Dans le système d'axes présenté, on peut écrire l'équation du mouvement~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum \overrightarrow{F}^{ext}=\overrightarrow{R}+\overrightarrow{P}+\overrightarrow{F}&=0\;\Rightarrow\\[0.8em]
|
||||||
|
F_x-R_x&=0\\
|
||||||
|
F_y+R_y-P&=0
|
||||||
|
\end{align*}
|
||||||
|
car le système est statique et l'accélération nulle.
|
||||||
|
|
||||||
|
En considérant que le poids \(P=m\cdot g\) et les triangles d'angles au sommet \(\alpha\) et \(\beta\), grâce à la trigonométrie, on peut écrire~:
|
||||||
|
\[F_x=F\cdot \cos(\beta)\;\;\textbf{et}\;\;R_x=R\cdot \cos(\alpha)\]
|
||||||
|
et préciser les équations du mouvement~:
|
||||||
|
\begin{align*}
|
||||||
|
F\cdot \cos(\beta)-R\cdot \cos(\alpha)&=0\\
|
||||||
|
F\cdot \sin(\beta)+R\cdot \sin(\alpha)-m\cdot g&=0
|
||||||
|
\end{align*}
|
||||||
|
Il s'agit de deux équations à deux inconnues F et R. Pour les résoudre, on tire F de la première et on la remplace dans la seconde~:
|
||||||
|
\begin{align*}
|
||||||
|
F&=R\cdot\frac{\cos(\alpha)}{\cos(\beta)}\;\;\Rightarrow\\
|
||||||
|
R&\cdot\frac{\cos(\alpha)}{\cos(\beta)}\cdot \sin(\beta)+R\cdot \sin(\alpha)-m\cdot g=0\;\Rightarrow\\
|
||||||
|
R&\cdot(\cos(\alpha)\cdot\tan(\beta)+\sin(\alpha))=m\cdot g\;\;\Rightarrow\\
|
||||||
|
R&=\frac{m\cdot g}{\cos(\alpha)\cdot\tan(\beta)+\sin(\alpha)}\\
|
||||||
|
&=\frac{7\cdot 9,81}{\cos(20)\cdot\tan(30)+\sin(20)}=\SI{77,63}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
et donc pour F~:
|
||||||
|
\begin{align*}
|
||||||
|
F&=R\cdot\frac{\cos(\alpha)}{\cos(\beta)}\\
|
||||||
|
&=77,63\cdot \frac{\cos(20)}{\cos(30)}=\SI{84,24}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{3}
|
||||||
|
On commence par choisir le système. Pour éviter de devoir calculer la tension dans la corde, on le choisit comme constitué de la corde et des deux masses M et m.
|
||||||
|
|
||||||
|
Les forces extérieures sont alors au nombre de trois. Le plan horizontal exerce sur la masse M une force de soutient verticale égale et opposée à son poids (mais qui ne sont pas l'action et la réaction l'une de l'autre), puisque la masse se déplace horizontalement. Ces deux forces s'annulent donc. Reste le poids de la masse m, seule force extérieure à agir pour accélérer le système.
|
||||||
|
|
||||||
|
On peut donc écrire, selon la seconde loi de Newton~:
|
||||||
|
\[\sum F^{ext}=m\cdot g=(M+m)\cdot a\]
|
||||||
|
où M+m est la masse du système. Ainsi, finalement, on peut calculer la valeur de l'accélération~:
|
||||||
|
\begin{align*}
|
||||||
|
&m\cdot g=(M+m)\cdot a\;\Rightarrow\\
|
||||||
|
&a=\frac{m}{M+m}\cdot g=\frac{2}{5}\cdot 9,81=\SI{3,924}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
\medskip
|
||||||
|
À partir de l'accélération, on peut ensuite calculer la vitesse au bout d'un mètre, grâce à l'équation du MRUA~:
|
||||||
|
\begin{align*}
|
||||||
|
v^2&=v_0^2+2\cdot a\cdot d\;\Rightarrow\\
|
||||||
|
v^2&=0+2\cdot 3,924\cdot 1\;\Rightarrow\\
|
||||||
|
v&=\sqrt{2\cdot 3,924}=\SI{2,8}{\metre\per\second}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{4}
|
||||||
|
Deux forces agissent ici~: la réaction du plan, qui lui est normale (c'est-à-dire perpendiculaire), et le poids de la masse. Comme la réaction du plan n'a aucune composante parallèlement au plan, elle ne peut être responsable de l'accélération de la masse le long de celui-ci.
|
||||||
|
|
||||||
|
Il faut donc trouver la composante du poids qui est parallèle au plan incliné. L'angle entre le poids et un plan horizontal est de \SI{90}{\degree}. Quand le plan est incliné, cet angle diminue de la valeur de l'inclinaison. L'angle \(\beta\) entre le plan incliné et le poids et donc \(\beta=90-\alpha\).
|
||||||
|
|
||||||
|
Comme la projection du poids selon l'angle \(\beta\) correspond à sa composante parallèle au plan, dans le triangle rectangle composé du poids comme hypoténuse et de ses composantes parallèle et perpendiculaire au plan, la composante parallèle au plan correspond au côté adjacent. Ainsi, on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
P_{//}&=P\cdot\cos(\beta)=P\cdot\cos(90-\alpha)\\
|
||||||
|
&=P\cdot\sin(\alpha)
|
||||||
|
\end{align*}
|
||||||
|
La seconde loi de Newton s'écrit donc le long du plan incliné~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}=P\cdot\sin(\alpha)&=m\cdot a\;\Rightarrow\\
|
||||||
|
m\cdot g\cdot\sin(\alpha)&=m\cdot a\;\Rightarrow\\
|
||||||
|
a&=g\cdot\sin(\alpha)\;\Rightarrow\\
|
||||||
|
a&=9,81\cdot\sin(20)=\SI{3,36}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
Avec une vitesse initiale nulle, pour un MRUA d'accélération calculée ci-dessus, la vitesse au bout d'un temps t=\SI{2}{\second} s'obtient par~:
|
||||||
|
\[v=a\cdot t+v_0=3,36\cdot 2=\SI{9,72}{\metre\per\second}\]
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Une autre manière de résoudre le problème est de procéder avec méthode. Le système qu'on doit choisir est bien évidemment la masse m, puisque c'est de celle-ci qu'on cherche l'accélération pour en trouver la vitesse au bout de \SI{2}{\second}.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Plan incliné]{Le plan incliné}\label{incline}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{5cm}
|
||||||
|
\input{Annexe-Exercices/Images/incline.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
|
||||||
|
La figure \ref{incline} présente ensuite le dessin des forces extérieures et le choix du système d'axes. Remarquez que ce dernier l'a été selon l'inclinaison du plan. Il aurait pu ne pas en être ainsi, mais ce choix simplifie les calculs, car la masse étant contrainte à se déplacer le long du plan, son accélération perpendiculairement est nulle. Les équations de la seconde loi de Newton, obtenues par projection des forces extérieures et de l'accélération selon les axes, peuvent alors s'écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}_x&=P_x=m\cdot a_x &\text{sur l'axe x}\\
|
||||||
|
\sum F^{ext}_y&=R-P_y=m\cdot a_y=0 &\text{sur l'axe y}
|
||||||
|
\end{align*}
|
||||||
|
car l'accélération perpendiculairement au plan est nulle, comme déjà mentionné.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Si on considère l'angle \(\alpha\), en s'imaginant le plan incliné horizontal, on comprends qu'il se reporte entre le vecteur poids \(\overleftarrow{P}\) et sa composante selon y \(P_y\).
|
||||||
|
|
||||||
|
Avec le triangle rectangle formé par le poids et ses composantes et un peu de trigonométrie, on peut en déduire~:
|
||||||
|
\begin{align*}
|
||||||
|
P_x &= P\cdot \sin(\alpha)\\
|
||||||
|
P_y &= P\cdot \cos(\alpha)
|
||||||
|
\end{align*}
|
||||||
|
Comme par ailleurs on sait que \(P=m\cdot g\), on peut réécrire les équations de Newton sur les axes comme~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}_x&=m\cdot g\cdot \sin(\alpha)=m\cdot a_x\\
|
||||||
|
\sum F^{ext}_y&=R-m\cdot g\cdot \cos(\alpha)=m\cdot a_y=0
|
||||||
|
\end{align*}
|
||||||
|
La première de ces équations permet de trouver l'accélération du bloc selon le plan incliné~:
|
||||||
|
\begin{align*}
|
||||||
|
a=a_x&=g\cdot \sin(\alpha)\\
|
||||||
|
&=9,81\cdot\sin(20)=\SI{3,36}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Mais une information supplémentaire nous est donnée par la seconde équation, c'est la valeur de la réaction R au plan~:
|
||||||
|
\begin{align*}
|
||||||
|
R&=m\cdot g\cdot \cos(\alpha)\\
|
||||||
|
&=3\cdot 9,81\cdot \cos(20)=\SI{27,67}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Ensuite, le problème se résout de la même manière que précédemment.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{5}
|
||||||
|
Le problème peut paraître complexe du fait de la présence de deux objets distincts se déplaçant selon deux axes différents. Pourtant, le fait que la corde soit inextensible fait de l'ensemble des deux masse et de la corde un système se déplaçant avec la même accélération. De plus, pour autant qu'on considère correctement l'action des forces sur chaque masse, on peut s'imaginer ce système se déplaçant d'un bloc horizontalement.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Comme on ne connaît pas la tension dans la corde (on ne peut s'imaginer à priori qu'elle correspond au poids de la masse m), le choix du système comprenant les deux masses et la corde s'impose, car ainsi la tension dans la corde, en tant que force intérieure, n'apparaîtra pas dans les équations de Newton.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Comme déjà dit, on peut considérer le système d'un seul tenant. On va donc imaginer un axe suivant la corde et orienté vers le bas du plan incliné, car la masse M étant plus grande que m, il est évident que le mouvement se fera dans ce sens. Ainsi, le signe de l'accélération sera positif.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Reste à considérer les forces extérieures. Elles sont au nombre de quatre~:
|
||||||
|
\begin{enumerate}
|
||||||
|
\item le poids P de la masse M,
|
||||||
|
\item la réaction R du plan incliné,
|
||||||
|
\item celui p de la masse et
|
||||||
|
\item la force exercée sur la corde par la poulie.
|
||||||
|
\end{enumerate}
|
||||||
|
|
||||||
|
La dernière est toujours perpendiculaire à la corde et ne participe donc pas au mouvement des masses. La troisième est toujours parallèle à la corde. La seconde est toujours perpendiculaire au plan incliné et ne participe elle aussi pas au mouvement. La première à une composante perpendiculaire au plan incliné et ne participe pas au mouvement, mais aussi une composante parallèle à ce plan et doit être considérée.
|
||||||
|
Avec l'angle \(\alpha\) défini, on peut reprendre le raisonnement évoqué au problème \ref{planinclinesimple}, évoquant le triangle rectangle formé par le poids de la masse M et se composantes et affirmant que l'angle \(\alpha\) est celui entre le poids et sa composante perpendiculaire au plan, pour écrire que la composante parallèle au plan vaut~:
|
||||||
|
\[P_{//}=M\cdot g\cdot \sin(\alpha)\]
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
À partir de là, on peut écrire l'équation du mouvement du système (des deux masse et de la corde)~:
|
||||||
|
\[\sum F^{ext}=M\cdot g\cdot \sin(\alpha)-m\cdot g=(M+m)\cdot a\]
|
||||||
|
et calculer l'accélération~:
|
||||||
|
\begin{align*}
|
||||||
|
a&=\frac{M\cdot g\cdot \sin(\alpha)-m\cdot g}{M+m}\\
|
||||||
|
&=\frac{5\cdot 9,81\cdot \sin(30)-3\cdot 9,81}{5+3}\\
|
||||||
|
&=\SI{-0,6}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
Le signe négatif signifie que la masse M monte vers le haut du plan incliné.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Pour calculer la tension dans la corde, il est indispensable de changer de système pour la faire apparaître en tant que force extérieure dans l'équation de Newton.
|
||||||
|
|
||||||
|
Trois éléments peuvent prétendre servir de système.
|
||||||
|
|
||||||
|
La corde en premier lieu. Si on la considère seule, à l'une de ses extrémités la masse m exerce sur elle une force \(T_m\) et à l'autre la masse M exerce une tension à priori différente \(T_M\). La force exercée par la poulie reste perpendiculaire et ne contribue pas au mouvement. On peut donc écrire~:
|
||||||
|
\[T_M-T_m=\mu\cdot a\]
|
||||||
|
où \(\mu\) est la masse de la corde. Or, si cette masse est nulle, indépendamment de l'accélération, le deux tensions sont égales. Cela est évidemment valable pour tous les éléments de la corde dont on dira donc qu'elle exerce une force \(T\) à déterminer.
|
||||||
|
|
||||||
|
Le système corde ne permet donc pas de la trouver.
|
||||||
|
|
||||||
|
Restent les deux masses. Pour la masse M interviendra dans l'équation du mouvement un sinus qu'on va éviter en considérant m.
|
||||||
|
|
||||||
|
Sur m, avec un axe pointant toujours vers le haut, l'équation de Newton devient très simple~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F{ext}&=T-m\cdot g=m\cdot a\;\Rightarrow\\
|
||||||
|
T&=m\cdot (a+g)=3\cdot (-0,6+9,81)\\
|
||||||
|
&=\SI{27,6}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Pour vérifier ce résultat, choisissons l'autre masse (M) pour système. On écrira alors~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}&=-T+M\cdot g\cdot \sin(\alpha)=M\cdot a\;\Rightarrow\\
|
||||||
|
T&=M\cdot g\cdot \sin(\alpha)-M\cdot a\\
|
||||||
|
&=5\cdot 9,81\cdot \sin(30)-5\cdot (-0,6)\\
|
||||||
|
&=\SI{27,6}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{6}
|
||||||
|
Pour calculer la vitesse de chute, il suffit de trouver la vitesse d'un objet en chute libre au bout de \SI{2}{\metre} de déplacement. Avec les équations du MRUA, on a~:
|
||||||
|
\begin{align*}
|
||||||
|
v&=\sqrt{2\cdot g\cdot h}=\sqrt{2\cdot 9.81\cdot 2}\\
|
||||||
|
&=\SI{6,26}{\metre\per\second}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
Ensuite, si on considère que la descente en parachute se fait à vitesse constante, c'est-à-dire avec une accélération nulle, on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}&=-T+m\cdot g=m\cdot a=0\;\Rightarrow\\
|
||||||
|
T&=m\cdot g=70\cdot 9,81=\SI{686,7}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
En d'autre termes, le parachute n'a à supporter que le poids du parachutiste.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{7}
|
||||||
|
\begin{enumerate}
|
||||||
|
\item Avec pour système la nacelle, la corde et la masse, les deux seules forces extérieures sont le poids P et la force exercée par le ballon F. Tout se déroulant sur un axe vertical, qu'on choisira vers le haut, on peut écrire la seconde loi sur cet axe~:
|
||||||
|
\[\sum F^{ext}=F-(M+m)\cdot g=(M+m)\cdot a=0\]
|
||||||
|
puisque l'accélération est nulle. Ainsi, la force F exercée par le ballon sur la nacelle est simplement égale au poids du système~:
|
||||||
|
\[F=(M+m)\cdot g=180\cdot 9,81=\SI{1765,8}{\newton}\]
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Le même raisonnement vaut pour la masse suspendue dont l'accélération est nulle. Ainsi la tension T dans la corde vaut exactement le poids de la masse pendante~:
|
||||||
|
\[T=m\cdot g=80\cdot 9,81=\SI{784,8}{\newton}\]
|
||||||
|
\item À vitesse constante, la force permettant au ballon de s'élever est donc égale au poids de ce qu'il soulève. La force d'ascension vaut donc \(F=\SI{1765,8}{\newton}\).
|
||||||
|
|
||||||
|
Si on lâche \SI{20}{\kilo\gram} de lest, la masse de la nacelle devient égale à \SI{80}{\kilo\gram}. La seconde loi de Newton permet alors de calculer l’accélération~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}&=F-(M+m)\cdot g=(M+m)\cdot a\;\Rightarrow\\
|
||||||
|
a&=\frac{F}{M+m}-g=\frac{1765,8}{80+80}-9,81\\
|
||||||
|
&=\SI{1,23}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
Évidemment, la force exercée par le ballon sur la nacelle vaut \SI{1765,8}{\newton}.
|
||||||
|
|
||||||
|
La force exercée par la corde sur la masse se calcule finalement par application de la seconde loi au système constitué uniquement de m~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum F^{ext}&=T-m\cdot g=m\cdot a\;\Rightarrow\\
|
||||||
|
T&=m\cdot a + m\cdot g=80\cdot (1,23+9,81)\\
|
||||||
|
&=\SI{882,9}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
\end{enumerate}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{8}
|
||||||
|
On verra ci-dessous que l'utilisation de la seconde loi de Newton permet d'obtenir une relation entre l'accélération de chaque masse, constituant une équation à deux inconnues. Pour déterminer la valeur des deux accélérations, il est donc nécessaire de trouver une seconde équation entre ces deux équations.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Imaginons une poulie suspendue à une corde qui dépasse de celle-ci des deux côtés d'une longueur L, comme présenté sur la figure \ref{cordepoulie}. La demi-circonférence de la poulie vaut aussi L.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Corde poulie]{Corde et poulie}\label{cordepoulie}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{2cm}
|
||||||
|
\input{Annexe-Exercices/Images/cordepoulie.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
On tire sur la corde à gauche pour la faire monter d'une hauteur L.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
La question est~: \emph{de quelle hauteur monte la poulie ?}
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Pour le déterminer, il faut considérer qu'en tirant sur la corde pour la faire monter d'une hauteur L, on amène le point A qui est à l'origine au contact de la poulie à la place du point B du haut de la corde (voir figure \ref{cordepoulie}). Si la poulie restait à sa place, on aurait la situation de la figure \ref{cordepoulietiree}). Mais, elle est en réalité libre de monter. Ce qui reste fixe est le point C de la figure \ref{cordepoulie}.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Corde tirée poulie]{Corde tirée et poulie}\label{cordepoulietiree}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{2cm}
|
||||||
|
\input{Annexe-Exercices/Images/cordepoulietiree.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
On a donc a répartir une longueur 2L de corde entre le point A de la figure \ref{cordepoulietiree} et le point C de la figure \ref{cordepoulie}. Comme la demi-circonférence de la poulie vaut L, il reste une longueur L à répartir des deux côtés de la poulie, soit L/2 de chaque côté, comme le montre la figure \ref{cordepoulietireejuste}.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Corde tirée poulie juste]{Corde tirée et poulie montée}\label{cordepoulietireejuste}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{3.1cm}
|
||||||
|
\input{Annexe-Exercices/Images/cordepoulietireejuste.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
Ainsi, quand on tire la corde d'une longueur L, la poulie monte d'une longueur L/2.
|
||||||
|
|
||||||
|
\bigskip
|
||||||
|
Pour revenir au système des deux poulies du problème, la remarque précédente se traduit par le fait que quand la masse m descend d'une longueur L, la masse M monte d'une longueur L/2.
|
||||||
|
|
||||||
|
L'accélération étant une distance divisée par un temps au carré, on comprends facilement que cela signifie que l'accélération de la masse m vaut simplement le double de celle de la masse M, soit~:
|
||||||
|
\[a_m=2\cdot a_M\]
|
||||||
|
Cette équation constitue une première relation entre les deux inconnues que sont les accélérations de chaque masse.
|
||||||
|
|
||||||
|
\bigskip
|
||||||
|
Les masses étant égales, on pourrait aussi croire que le système est en équilibre. Ce n'est pas le cas. Pour le comprendre, considérons la poulie qui n'est pas accrochée au plafond.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
À l'instar d'une poulie suspendue au plafond à laquelle on accroche deux masses identiques pendantes par l'intermédiaire d'une corde, la force totale qu'exerce sur elle le plafond vaut évidemment le poids total des deux masses, puisque la poulie ne bouge pas. Or, pour que chaque masse individuellement ne bouge pas, il faut que la corde qui passe dans la poulie exerce sur chacune d'elle une force égale à son poids. De chaque côté de la poulie, la corde exerce donc une même force et la poulie est tirée vers le bas par l'ensemble de ces deux forces.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Ainsi, sur la poulie qui n'est pas accrochée au plafond, la force totale exercée vers le haut vaut deux fois la tension dans la corde. Vers le bas, seule le poids de la masse M qui lui est suspendue est présent.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
De l'autre côté, la masse m retenue par la corde qui passe sur la poulie suspendue au plafond est soumise à un poids identique vers le bas et à une seule force vers le haut exercée par la corde. Comme la masse de la corde est nulle, la tension dans la corde est la même partout.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
Finalement, la masse M est tirée vers le haut par deux fois la tension dans la corde et la masse m est retenue par une fois la tension dans la corde. Clairement donc, la première monte et la seconde descend.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Le choix du système d'axe est donc clair~: vers le haut pour la masse M qui monte et vers le bas pour m qui descend, le mouvement se faisant dans cette direction avec une accélération a identique pour les deux masses.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
On peut alors écrire les équations du mouvement de chaque masse ainsi~:
|
||||||
|
\begin{align*}
|
||||||
|
m\cdot g-T&=m\cdot a_m\\
|
||||||
|
2\cdot T-M\cdot g&=M\cdot a_M
|
||||||
|
\end{align*}
|
||||||
|
En multipliant par deux la première équation, on peut les additionner pour en tirer l'accélération.
|
||||||
|
\begin{align*}
|
||||||
|
2\cdot m\cdot g-2\cdot T&=2\cdot m\cdot a_m\\
|
||||||
|
+\;\;\;\;\;\;\;\;\;\;2\cdot T-M\cdot g&=M\cdot a_M\\
|
||||||
|
\hline\\
|
||||||
|
2\cdot m\cdot g-M\cdot g&=2\cdot m\cdot a_m+M\cdot a_M
|
||||||
|
\end{align*}
|
||||||
|
Cela constitue la seconde relation entre les deux inconnues que sont les accélérations de chaque masse.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
Avec la première relation établie ci-dessus entre les accélérations des deux masses (\(a_m=2\cdot a_M\)), on a alors~:
|
||||||
|
\begin{align*}
|
||||||
|
2\cdot m\cdot g-M\cdot g&=2\cdot m\cdot a_m+M\cdot a_M\;\Rightarrow\\
|
||||||
|
2\cdot m\cdot g-M\cdot g&=2\cdot m\cdot 2\cdot a_M+M\cdot a_M\;\Rightarrow\\
|
||||||
|
2\cdot m\cdot g-M\cdot g&=4\cdot m\cdot a_M+M\cdot a_M\;\Rightarrow\\
|
||||||
|
a_M&=\frac{2\cdot m-M}{4\cdot m+M}\cdot g
|
||||||
|
\end{align*}
|
||||||
|
Dans le cas où les deux masse sont identiques (M=m), on a alors~:
|
||||||
|
\[a_M=\frac{2\cdot m-m}{4\cdot m+m}\cdot g=\frac{m}{5\cdot m}\cdot g=\frac{1}{5}\cdot g\]
|
||||||
|
et pour l'accélération de m~:\[a_m=2\cdot a_M=\frac{2}{5}\cdot g\]
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{9}
|
||||||
|
Dans ce problème, on n'utilise pas le système d'axes de la figure \ref{incline} qui est parallèle et normal au plan incliné, mais un système d'axes horizontal et vertical. Les équations du mouvement selon ce système s'écrivent avec des notations évidentes~:
|
||||||
|
\begin{align*}
|
||||||
|
\sum \overrightarrow{F}^{ext}=\overrightarrow{R}+\overrightarrow{P}&=m\cdot \overrightarrow{a}\;\;\Rightarrow\\[0.8em]
|
||||||
|
R_x&=m\cdot a_x\\
|
||||||
|
R_y-P&=m\cdot a_y
|
||||||
|
\end{align*}
|
||||||
|
En considérant que l'angle \(\alpha\) du plan incliné se retrouve entre la réaction R et la verticale, on peut écrire~:
|
||||||
|
\[R_x=R\cdot \sin(\alpha)\;\;\text{et}\;\;R_y=R\cdot \cos(\alpha)\]
|
||||||
|
et finalement en tirer les accélérations cherchées~:
|
||||||
|
\begin{align*}
|
||||||
|
a_x&=\frac{R\cdot \sin(\alpha)}{m}\\
|
||||||
|
a_y&=\frac{R\cdot \cos(\alpha)-m\cdot g}{m}
|
||||||
|
\end{align*}
|
||||||
|
Visiblement, on a deux équations pour trois inconnues, les deux accélérations et la réaction du plan.
|
||||||
|
|
||||||
|
Pour le calcul de cette dernière, il est donc nécessaire de disposer de l'équation supplémentaire donnée par la contrainte imposée à la masse de rester sur le plan incliné, soit la relation spécifiant que la réaction R est égale à la composante perpendiculaire au plan incliné du poids~:
|
||||||
|
\[R=P\cdot \cos(\alpha)=m\cdot g\cdot \cos(\alpha)\]
|
||||||
|
Ainsi, en remplaçant dans les équations du mouvement, on a~:
|
||||||
|
\begin{align*}
|
||||||
|
a_x&=\frac{m\cdot g\cdot \cos(\alpha)\cdot \sin(\alpha)}{m}\\
|
||||||
|
a_y&=\frac{m\cdot g\cdot \cos^2(\alpha)-m\cdot g}{m}\\[0.8em]
|
||||||
|
a_x&=g\cdot\cos(\alpha)\sin(\alpha)\\
|
||||||
|
a_y&=g\cdot (\cos^2(\alpha)-1)=-g\cdot\sin^2(\alpha)
|
||||||
|
\end{align*}
|
||||||
|
Pour vérifier que ces relations sont correctes, on peut calculer la norme du vecteur accélération qui devrait selon le problème \ref{planinclinesimple} valoir \(a=g\sin(\alpha)\). Le calcul est le suivant~:
|
||||||
|
\begin{align*}
|
||||||
|
a&=\sqrt{a_x^2+a_y^2}\\
|
||||||
|
&=\sqrt{(g\cdot\cos(\alpha)\sin(\alpha))^2+(-g\cdot\sin^2(\alpha)^2}\\
|
||||||
|
&=\sqrt{g^2\cdot\cos^2(\alpha)\sin^2(\alpha)+g^2\cdot\sin^4(\alpha)}\\
|
||||||
|
&=\sqrt{g^2\cdot\sin^2(\alpha)\cdot (\cos^2(\alpha)+\sin^2(\alpha))}\\
|
||||||
|
&=\sqrt{g^2\cdot\sin^2(\alpha)}\\
|
||||||
|
&=g\cdot\sin(\alpha)
|
||||||
|
\end{align*}
|
||||||
|
Ce qu'il fallait démontrer.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{10}
|
||||||
|
Rappelons tout d'abord que l'exercice \ref{massesuspendue} a permis de calculer l'accélération d'un système de deux masses, l'une sur un plan horizontal, la masse M', et l'autre pendant dans le vide, la masse m, accrochée à la première par une ficelle sans masse. Avec un système constitué des deux masses, on a pu montrer que~:
|
||||||
|
\[m\cdot g=(M'+m)\cdot a\;\;\Rightarrow\;\;a=\frac{m}{M'+m}\cdot g\]
|
||||||
|
|
||||||
|
C'est à partir de là que l'on peut résoudre le présent problème.
|
||||||
|
|
||||||
|
\smallskip
|
||||||
|
La solution est toute simple. À un instant donné on groupe toute la masse qui glisse sur le plan pour en faire la masse M et toute la masse pendante pour en faire la masse m. Pour cela, définissons une masse par unité de longueur de corde~:
|
||||||
|
\[\rho=\frac{M}{L}\]
|
||||||
|
Ainsi on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
M&=(L-y)\cdot \rho=(L-y)\cdot\frac{M}{L}\\
|
||||||
|
m&=y\cdot \rho=y\cdot\frac{M}{L}
|
||||||
|
\end{align*}
|
||||||
|
Ainsi, on peut simplement écrire l'équation de l’accélération~:
|
||||||
|
\begin{align*}
|
||||||
|
a&=\frac{m}{M+m}\cdot g=\frac{y\cdot M/L}{(L-y)\cdot M/L+y\cdot M/L}\cdot g\\
|
||||||
|
&=\frac{y}{(L-y)+y}\cdot g=\frac{y}{L}\cdot g
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{11}
|
||||||
|
On commence par calculer l'accélération à la surface de Sedna grâce à la loi de la gravitation universelle~:
|
||||||
|
\begin{align*}
|
||||||
|
g_{Sedna}&=G\cdot \frac{M}{R^2}=6,67\cdot 10^{-11}\cdot \frac{10^{21}}{(995\cdot 10^3/2)^2}\\
|
||||||
|
&=\SI{0,27}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
On peut alors calculer les deux poids~:
|
||||||
|
\begin{align*}
|
||||||
|
P_{Terre}&=m\cdot g=13\cdot 9,81=\SI{127,5}{\newton}\\
|
||||||
|
P_{Sedna}&=m\cdot g=13\cdot 0,27=\SI{3,5}{\newton}\\
|
||||||
|
\end{align*}
|
||||||
|
Le rapport est alors de 127,5/3,5=36,4.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{12}
|
||||||
|
La seconde loi de Newton pour la trajectoire circulaire d'un corps m soumis à la gravitation autour d'une masse centrale M s'écrit~:
|
||||||
|
\[G\cdot \frac{M\cdot m}{r^2}=m\cdot a=m\cdot \frac{v^2}{r}\]
|
||||||
|
Sur une trajectoire circulaire la vitesse vaut~:
|
||||||
|
\[v=\frac{2\cdot \pi\cdot r}{T}\]
|
||||||
|
où T est la période de rotation de la masse m. Ainsi, on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
G\cdot \frac{M\cdot m}{r^2}&=m\cdot \frac{(2\cdot \pi r)^2}{T^2\cdot r}\\
|
||||||
|
G\cdot \frac{M}{r^2}&=\frac{4\cdot \pi^2\cdot r}{T^2}\;\Rightarrow\\
|
||||||
|
M&=\frac{4\cdot \pi^2\cdot r^3}{G\cdot T^2}
|
||||||
|
\end{align*}
|
||||||
|
Avec les données suivantes~:
|
||||||
|
\begin{align*}
|
||||||
|
r&=5,91\cdot 11,19\cdot 6,371\cdot 10^6=\SI{421,33e6}{\metre}\\
|
||||||
|
T&=1,769\cdot 24\cdot 3'600=\SI{1,53e5}{\second}
|
||||||
|
\end{align*}
|
||||||
|
on peut alors calculer la masse~:
|
||||||
|
\begin{align*}
|
||||||
|
M&=\frac{4\cdot \pi^2\cdot r^3}{G\cdot T^2}\\
|
||||||
|
&=\frac{4\cdot \pi^2\cdot (421,33\cdot 10^6)^3}{6,67\cdot 10^{-11}\cdot (1,53\cdot 10^5)^2}\\
|
||||||
|
&=\SI{1,89e27}{\kilo\gram}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{13}
|
||||||
|
La situation est celle de la figure \ref{inclinefrottement}.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Frottements]{Frottements sur plan incliné}\label{inclinefrottement}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{5cm}
|
||||||
|
\input{Annexe-Exercices/Images/inclinefrottement.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
Dans le système d'axe de cette figure, les équations du mouvement sont~:
|
||||||
|
\begin{align*}
|
||||||
|
P_x-F_f=m\cdot a\\
|
||||||
|
R-P_y=0
|
||||||
|
\end{align*}
|
||||||
|
Si le bloc est statique, l'accélération est nulle, la force de frottement vaut~:
|
||||||
|
\[F_f=\mu_0\cdot R\]
|
||||||
|
et les composantes du poids sont~:
|
||||||
|
\[P_x=P\cdot \sin(\alpha)\;\;\textbf{et}\;\;P_y=P\cdot \cos(\alpha)\]
|
||||||
|
Ainsi, les équations du mouvement deviennent~:
|
||||||
|
\begin{align*}
|
||||||
|
P\cdot \sin(\alpha)-\mu_0\cdot R=0\\
|
||||||
|
R-P\cdot \cos(\alpha)=0
|
||||||
|
\end{align*}
|
||||||
|
En remplaçant la réaction R de la seconde équation dans la première, on obtient~:
|
||||||
|
\begin{align*}
|
||||||
|
P\cdot \sin(\alpha)&-\mu_0\cdot P\cdot \cos(\alpha)=0\;\;\Rightarrow\\
|
||||||
|
P\cdot \sin(\alpha)&=\mu_0\cdot P\cdot \cos(\alpha)\;\;\Rightarrow\\
|
||||||
|
\mu_0=\frac{\sin(\alpha)}{\cos(\alpha)}&=\tan(\alpha)=\tan(32)=\SI{0,62}{}
|
||||||
|
\end{align*}
|
||||||
|
\smallskip
|
||||||
|
Si le bloc glisse, c'est le c\oe fficient cinétique qui intervient dans la force de frottement. Celui-ci vaut~:
|
||||||
|
\[\mu=(1-0,05)\cdot \mu_0=0,95\cdot 0,62=\SI{0,59}{}\]
|
||||||
|
Alors, sur l'axe x, avec la composante du poids parallèle au plan incliné et la force de frottement proportionnelle à la réaction R égale à la composante du poids perpendiculaire au plan, on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
m&\cdot g\cdot \sin(\alpha)-\mu\cdot m\cdot g\cdot \cos(\alpha)=m\cdot a\;\;\Rightarrow\\
|
||||||
|
a&=g\cdot (\sin(\alpha)-\mu\cdot \cos(\alpha))\\
|
||||||
|
&=9,81\cdot (\sin(32)-0,59\cdot \cos(32))=\SI{0,29}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{14}
|
||||||
|
Tant que les deux blocs ne glissent pas, la force de frottement est statique. Si on considère comme système le bloc supérieur, celui-ci étant immobile sur le bloc inférieur, la forces F et celle de frottement s'annulent. Elles sont donc égales et si la force F exercée sur le bloc supérieur augmente, la force de frottement statique augmente également dans une exacte mesure. Cela jusqu'à la valeur de frottement statique maximum exercée par m sur M, donnée par l'équation~:
|
||||||
|
\begin{align*}
|
||||||
|
F&=F_{fr\:stat\:max}=\mu\cdot N=\mu\cdot m\cdot g\\
|
||||||
|
&=0,6\cdot 2\cdot 9,81=\SI{11,77}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
On est alors à l'imminence de glissement.
|
||||||
|
|
||||||
|
Pour calculer l'accélération des deux masses, qui n'en forment alors plus qu'une, il faut choisir le système qui les constitue et écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
F&=(M+m)\cdot a\;\Rightarrow\;a=\frac{F}{M+m}\\
|
||||||
|
&=\frac{11,77}{2+5}=\SI{1,68}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
À partir du moment où le glissement commence, la force de frottement statique maximum devient une force de frottement cinétique. Si les c\oe fficients de frottements statique et cinétique sont égaux, la force de frottement cinétique est égale à celle statique maximale et ne varie plus. Ainsi, sur le bloc du bas ne s'exerce qu'une seule force extérieure, c'est la réaction à la force de frottement cinétique exercée par le bloc du bas sur celui du haut. Sa valeur est donnée par le calcul ci-dessus. Ainsi, on peut écrire pour le système du bas~:
|
||||||
|
\begin{align*}
|
||||||
|
F_{fr\:stat\:max}&=M\cdot a_M\;\Rightarrow\\
|
||||||
|
a_M&=\frac{11,77}{5}=\SI{2,35}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
Quant au bloc du haut, deux forces extérieures s'exercent sur lui~: la force F et la force de frottement dynamique, égale à la force de frottement statique maximale. Pour ce système, on peut écrire~:
|
||||||
|
\begin{align*}
|
||||||
|
F-F_{fr\:stat\:max}&=m\cdot a_m\;\Rightarrow\\
|
||||||
|
a_m&=\frac{23,54-11,77}{2}=\SI{5,89}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{15}
|
||||||
|
Les deux forces de frottement statique et cinétique valent~:
|
||||||
|
\begin{align*}
|
||||||
|
F_{fr\:stat\:max}&=\mu_{stat}\cdot m\cdot g\\
|
||||||
|
&=0,6\cdot 20'000\cdot 9,81=\SI{117720}{\newton}\\
|
||||||
|
F_{cin}&=\mu_{cin}\cdot m\cdot g\\
|
||||||
|
&=0,4\cdot 20'000\cdot 9,81=\SI{78480}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
Les deux décélérations sont alors~:
|
||||||
|
\begin{align*}
|
||||||
|
-F_{fr\:stat\:max}&=m\cdot a_{stat}\;\Rightarrow\\
|
||||||
|
a_{stat}&=\frac{-117'720}{20'000}=\SI{-5,886}{\metre\per\second\squared}\\
|
||||||
|
-F_{cin}&=m\cdot a_{cin}\;\Rightarrow\\
|
||||||
|
a_{cin}&=\frac{-78'480}{20'000}=\SI{-3,924}{\metre\per\second\squared}
|
||||||
|
\end{align*}
|
||||||
|
On peut alors calculer la distance de freinage dans chaque cas~:
|
||||||
|
\begin{align*}
|
||||||
|
v^2&=v_0^2+2\cdot a\cdot d\;\Rightarrow\;d=\frac{v^2-v_0^2}{2\cdot a}\\
|
||||||
|
d_{stat}&=\frac{0-13,89^2}{2\cdot (-5,886)}=\SI{16,39}{\metre}\\
|
||||||
|
d_{cin}&=\frac{0-13,89^2}{2\cdot (-3,924)}=\SI{24,58}{\metre}
|
||||||
|
\end{align*}
|
||||||
|
La différence est donc de \(24,58-16,39=\SI{8,19}{\metre}\).
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{16}
|
||||||
|
Le poids du bloc de masse m vaut~:
|
||||||
|
\[P_m=m\cdot g=3\cdot 9,81=\SI{29,43}{\newton}\]
|
||||||
|
Pour que ce bloc ne tombe pas, il faut qu'une force verticale s'exerce vers le haut et compense le poids calculé ci-dessus, soit \(F_{fr}=P\). L'origine de cette force est évidemment le frottement entre les deux blocs. Or, celle-ci dépend de la force exercée par la masse M sur m, notée \(\overrightarrow{N}\), qui joue le rôle de la réaction R du sol pour un objet glissant horizontalement. La figure \ref{blocsuspenduforces} présente la situation qui permet d'exprimer la force de frottement et de déterminer la valeur N de la réaction.
|
||||||
|
\begin{figure}[ht]
|
||||||
|
\centering
|
||||||
|
\caption[Forces sur bloc suspendu]{Forces sur le bloc suspendu}\label{blocsuspenduforces}
|
||||||
|
\medskip
|
||||||
|
\def\svgwidth{4cm}
|
||||||
|
\input{Annexe-Exercices/Images/blocsuspenduforces.eps_tex}
|
||||||
|
\end{figure}
|
||||||
|
\begin{align*}
|
||||||
|
F_{fr}&=\mu_{stat}\cdot N\;\Rightarrow\\
|
||||||
|
N&=\frac{F_{fr}}{\mu_{stat}}=\frac{29,43}{0,5}=\SI{58,86}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
On peut dire en français que pour avoir une force de frottement donnée il faut une réaction normale N de valeur double, en raison du c\oe fficient de frottement particulier ici.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
C'est la force normale \(\overrightarrow{N}\) qui est la seule force qui pousse la masse m horizontalement. Elle est donc responsable de l'accélération qu'on peut ainsi calculer simplement à l'aide de la seconde loi~:
|
||||||
|
\[a=\frac{N}{m}=\frac{58,56}{3}=\SI{19,62}{\metre\per\second\squared}\]
|
||||||
|
Cette accélération est celle de la masse m, mais aussi de M. La valeur F de la force permettant de l'obtenir pour le système constitué par les deux masses est donc finalement~:
|
||||||
|
\[F=(M+m)\cdot a=7\cdot 19,62=\SI{137,34}{\newton}\]
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{17}
|
||||||
|
Un autre corrigé de test.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{18}
|
||||||
|
Un autre corrigé de test.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{19}
|
||||||
|
Un autre corrigé de test.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
|
\begin{Solution OS}{20}
|
||||||
|
Le travail de l'équipe pour remonter le bobsleigh du bas de la piste à son point de départ sert à augmenter l'énergie potentielle du bob. On néglige les frottement exercés sur le véhicule de transport. Ainsi, on a~:
|
||||||
|
\begin{align*}
|
||||||
|
E_{pot}&=m\cdot g\cdot h=250\cdot 9,81\cdot (1000-800)\\
|
||||||
|
&=\SI{490500}{\joule}
|
||||||
|
\end{align*}
|
||||||
|
pour une seule montée. Pour 5 montées, on a donc \SI{2452500}{\joule}.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
C'est évidemment la même énergie qui est perdue pendant la descente (à l'exception de la poussée initiale). Elle vient du travail du poids sur le bob et les quatre personnes qui se trouvent à l'intérieur.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
L'énergie potentielle perdue par le bob sert à augmenter sa vitesse et à lutter contre le frottement. Le travail nécessaire à parvenir à une vitesse de \SI{80}{\kilo\metre\per\hour} est égal à l'énergie cinétique acquise. Pour un bob de \SI{600}{\kilo\gram} et une vitesse moyenne de 80/3,6=\SI{22,2}{\metre\per\second}, on a un travail de~:
|
||||||
|
\[A=\frac{1}{2}\cdot m\cdot v^2=\frac{1}{2}\cdot 600\cdot 22,2^2=\SI{148148}{\joule}\]
|
||||||
|
par descente. Soit au total, pour 5 descentes \SI{740740}{\joule}.
|
||||||
|
|
||||||
|
Cette valeur est supérieure à l'énergie fournie au bob pendant la montée. C'est normal, car on a pas tenu compte alors de l'énergie nécessaire à monter les personnes. Pour cela, il faut calculer l'énergie potentielle acquise par la masse de \SI{600}{\kilo\gram}~:
|
||||||
|
\[E_{pot}=600\cdot 9,81\cdot 200=\SI{1177200}{\joule}\]
|
||||||
|
qui est bien supérieure à celle fournie pour augmenter la vitesse.
|
||||||
|
|
||||||
|
\medskip
|
||||||
|
La différence d'énergie potentielle et cinétique, soit 1'117'200-740'740 = \SI{436460}{\joule}, est perdue dans le frottement.
|
||||||
|
|
||||||
|
Comme la distance sur laquelle il s'exerce est de \SI{1800}{\metre}, on peut calculer la force de frottement moyenne par~:
|
||||||
|
\begin{align*}
|
||||||
|
A_{fr}&=F_fr\cdot d\;\Rightarrow\\
|
||||||
|
F_{fr}&=\frac{A_{fr}}{d}=\frac{436'460}{1'800}=\SI{242,5}{\newton}
|
||||||
|
\end{align*}
|
||||||
|
C'est évidemment une estimation.
|
||||||
|
|
||||||
|
\end{Solution OS}
|
||||||
@ -1,52 +1,52 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {5}Thermodynamique}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {10}Thermodynamique}{129}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\newlabel{chapthermo}{{5}{91}}
|
\newlabel{chapthermo}{{10}{129}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.1}Introduction}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {10.1}Introduction}{129}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.2}Temp\IeC {\'e}rature}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {10.2}Temp\IeC {\'e}rature}{129}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.1}Celsius}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.2.1}Celsius}{129}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.2}Fahrenheit}{91}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.2.2}Fahrenheit}{129}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.3}Kelvin}{92}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.2.3}Kelvin}{130}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.2.4}Agitation mol\IeC {\'e}culaire}{92}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.2.4}Agitation mol\IeC {\'e}culaire}{130}\protected@file@percent }
|
||||||
\newlabel{vitair}{{5.1}{92}}
|
\newlabel{vitair}{{10.1}{130}}
|
||||||
\newlabel{celsiusfahrenheit}{{5.1(a)}{92}}
|
\newlabel{celsiusfahrenheit}{{10.1(a)}{130}}
|
||||||
\newlabel{sub@celsiusfahrenheit}{{(a)}{92}}
|
\newlabel{sub@celsiusfahrenheit}{{(a)}{130}}
|
||||||
\newlabel{celsiuskelvin}{{5.1(b)}{92}}
|
\newlabel{celsiuskelvin}{{10.1(b)}{130}}
|
||||||
\newlabel{sub@celsiuskelvin}{{(b)}{92}}
|
\newlabel{sub@celsiuskelvin}{{(b)}{130}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.1}{\ignorespaces Thermom\IeC {\`e}tres}}{92}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {10.1}{\ignorespaces Thermom\IeC {\`e}tres}}{130}\protected@file@percent }
|
||||||
\newlabel{thermometres}{{5.1}{92}}
|
\newlabel{thermometres}{{10.1}{130}}
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Fahrenheit}}}{92}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Fahrenheit}}}{130}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Kelvin}}}{92}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Kelvin}}}{130}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.3}Dilatation}{92}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {10.3}Dilatation}{130}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {5.1}{\ignorespaces C\oe fficient de dilatation lin\IeC {\'e}aire\relax }}{93}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {10.1}{\ignorespaces C\oe fficient de dilatation lin\IeC {\'e}aire\relax }}{131}\protected@file@percent }
|
||||||
\newlabel{coefdilat}{{5.1}{93}}
|
\newlabel{coefdilat}{{10.1}{131}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.4}Chaleur}{93}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {10.4}Chaleur}{131}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.4.1}Chaleur sp\IeC {\'e}cifique}{93}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.4.1}Chaleur sp\IeC {\'e}cifique}{131}\protected@file@percent }
|
||||||
\newlabel{thermique}{{5.3}{93}}
|
\newlabel{thermique}{{10.3}{131}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {5.2}{\ignorespaces Chaleur sp\IeC {\'e}cifique\relax }}{93}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {10.2}{\ignorespaces Chaleur sp\IeC {\'e}cifique\relax }}{131}\protected@file@percent }
|
||||||
\newlabel{tabchalspe}{{5.2}{93}}
|
\newlabel{tabchalspe}{{10.2}{131}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.4.2}Chaleur latente}{93}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.4.2}Chaleur latente}{131}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.2}{\ignorespaces Changements d'\IeC {\'e}tats\relax }}{94}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {10.2}{\ignorespaces Changements d'\IeC {\'e}tats\relax }}{132}\protected@file@percent }
|
||||||
\newlabel{paliers}{{5.2}{94}}
|
\newlabel{paliers}{{10.2}{132}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {5.3}{\ignorespaces Chaleur latente\relax }}{94}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {10.3}{\ignorespaces Chaleur latente\relax }}{132}\protected@file@percent }
|
||||||
\newlabel{tabchaleurlat}{{5.3}{94}}
|
\newlabel{tabchaleurlat}{{10.3}{132}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {5.5}\IeC {\'E}nergie thermique}{94}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {10.5}\IeC {\'E}nergie thermique}{132}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {5.5.1}Premier principe}{95}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {10.5.1}Premier principe}{133}\protected@file@percent }
|
||||||
\newlabel{premierprincipe}{{5.5}{95}}
|
\newlabel{premierprincipe}{{10.5}{133}}
|
||||||
\newlabel{RF4}{96}
|
\newlabel{RF4}{134}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {5.3}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de thermodynamique\relax }}{96}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {10.3}{\ignorespaces R\IeC {\'e}sum\IeC {\'e} de thermodynamique\relax }}{134}\protected@file@percent }
|
||||||
\@setckpt{Thermodynamique/Thermodynamique}{
|
\@setckpt{Thermodynamique/Thermodynamique}{
|
||||||
\setcounter{page}{97}
|
\setcounter{page}{135}
|
||||||
\setcounter{equation}{11}
|
\setcounter{equation}{11}
|
||||||
\setcounter{enumi}{7}
|
\setcounter{enumi}{2}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
\setcounter{enumiii}{0}
|
\setcounter{enumiii}{0}
|
||||||
\setcounter{enumiv}{0}
|
\setcounter{enumiv}{0}
|
||||||
\setcounter{footnote}{0}
|
\setcounter{footnote}{0}
|
||||||
\setcounter{mpfootnote}{0}
|
\setcounter{mpfootnote}{0}
|
||||||
\setcounter{part}{0}
|
\setcounter{part}{0}
|
||||||
\setcounter{chapter}{5}
|
\setcounter{chapter}{10}
|
||||||
\setcounter{section}{5}
|
\setcounter{section}{5}
|
||||||
\setcounter{subsection}{1}
|
\setcounter{subsection}{1}
|
||||||
\setcounter{subsubsection}{0}
|
\setcounter{subsubsection}{0}
|
||||||
@ -59,7 +59,7 @@
|
|||||||
\setcounter{parentequation}{0}
|
\setcounter{parentequation}{0}
|
||||||
\setcounter{FancyVerbLine}{0}
|
\setcounter{FancyVerbLine}{0}
|
||||||
\setcounter{float@type}{8}
|
\setcounter{float@type}{8}
|
||||||
\setcounter{fignum}{0}
|
\setcounter{fignum}{1}
|
||||||
\setcounter{r@tfl@t}{4}
|
\setcounter{r@tfl@t}{4}
|
||||||
\setcounter{subfigure}{0}
|
\setcounter{subfigure}{0}
|
||||||
\setcounter{lofdepth}{1}
|
\setcounter{lofdepth}{1}
|
||||||
@ -67,7 +67,7 @@
|
|||||||
\setcounter{lotdepth}{1}
|
\setcounter{lotdepth}{1}
|
||||||
\setcounter{caption@flags}{0}
|
\setcounter{caption@flags}{0}
|
||||||
\setcounter{ContinuedFloat}{0}
|
\setcounter{ContinuedFloat}{0}
|
||||||
\setcounter{endnote}{51}
|
\setcounter{endnote}{55}
|
||||||
\setcounter{OptionTest}{0}
|
\setcounter{OptionTest}{0}
|
||||||
\setcounter{DefaultLines}{2}
|
\setcounter{DefaultLines}{2}
|
||||||
\setcounter{DefaultDepth}{0}
|
\setcounter{DefaultDepth}{0}
|
||||||
|
|||||||
@ -1,173 +1,173 @@
|
|||||||
\relax
|
\relax
|
||||||
\@writefile{toc}{\contentsline {chapter}{\numberline {11}Thermodynamique}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {chapter}{\numberline {11}Thermodynamique}{135}\protected@file@percent }
|
||||||
\@writefile{lof}{\addvspace {10\p@ }}
|
\@writefile{lof}{\addvspace {10\p@ }}
|
||||||
\@writefile{lot}{\addvspace {10\p@ }}
|
\@writefile{lot}{\addvspace {10\p@ }}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.1}Temp\IeC {\'e}rature et dilatation}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.1}Temp\IeC {\'e}rature et dilatation}{135}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.1.1}Temp\IeC {\'e}rature}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.1.1}Temp\IeC {\'e}rature}{135}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.1.2}Dilatation}{139}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.1.2}Dilatation}{135}\protected@file@percent }
|
||||||
\newlabel{dilatation}{{11.1.2}{139}}
|
\newlabel{dilatation}{{11.1.2}{135}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.1}{\ignorespaces Dilatation lin\IeC {\'e}aire\relax }}{140}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.1}{\ignorespaces Dilatation lin\IeC {\'e}aire\relax }}{136}\protected@file@percent }
|
||||||
\newlabel{dilatationlineaire}{{11.1}{140}}
|
\newlabel{dilatationlineaire}{{11.1}{136}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.1}{\ignorespaces Coefficient de dilatation lin\IeC {\'e}aire\relax }}{140}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.1}{\ignorespaces Coefficient de dilatation lin\IeC {\'e}aire\relax }}{136}\protected@file@percent }
|
||||||
\newlabel{coefflineaire}{{11.1}{140}}
|
\newlabel{coefflineaire}{{11.1}{136}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.2}{\ignorespaces Fusible bilame\relax }}{140}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.2}{\ignorespaces Fusible bilame\relax }}{136}\protected@file@percent }
|
||||||
\newlabel{bilame}{{11.2}{140}}
|
\newlabel{bilame}{{11.2}{136}}
|
||||||
\newlabel{gamma}{{11.2}{140}}
|
\newlabel{gamma}{{11.2}{136}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.3}{\ignorespaces Dilatation volumique\relax }}{141}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.3}{\ignorespaces Dilatation volumique\relax }}{137}\protected@file@percent }
|
||||||
\newlabel{dilatationvolumique}{{11.3}{141}}
|
\newlabel{dilatationvolumique}{{11.3}{137}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.2}{\ignorespaces Coefficient de dilatation volumique\relax }}{141}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.2}{\ignorespaces Coefficient de dilatation volumique\relax }}{137}\protected@file@percent }
|
||||||
\newlabel{coeffvolume}{{11.2}{141}}
|
\newlabel{coeffvolume}{{11.2}{137}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.2}Chaleurs sp\IeC {\'e}cifique et latente}{141}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.2}Chaleurs sp\IeC {\'e}cifique et latente}{137}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.1}Introduction}{141}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.1}Introduction}{137}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.2}Chaleur sp\IeC {\'e}cifique}{141}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.2}Chaleur sp\IeC {\'e}cifique}{137}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Chaleur massique}{141}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Chaleur massique}{137}\protected@file@percent }
|
||||||
\newlabel{ParaChaleurMassique}{{11.2.2}{141}}
|
\newlabel{ParaChaleurMassique}{{11.2.2}{137}}
|
||||||
\newlabel{chaleurmassique}{{11.4}{141}}
|
\newlabel{chaleurmassique}{{11.4}{137}}
|
||||||
\newlabel{Qchaleurmassique}{{11.5}{142}}
|
\newlabel{Qchaleurmassique}{{11.5}{138}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.3}{\ignorespaces Chaleur massique\relax }}{142}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.3}{\ignorespaces Chaleur massique\relax }}{138}\protected@file@percent }
|
||||||
\newlabel{tabchaleurmassique}{{11.3}{142}}
|
\newlabel{tabchaleurmassique}{{11.3}{138}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Capacit\IeC {\'e} thermique}{142}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Capacit\IeC {\'e} thermique}{138}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Notion de mole}{142}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Notion de mole}{138}\protected@file@percent }
|
||||||
\newlabel{Avogadro}{{11.6}{142}}
|
\newlabel{Avogadro}{{11.6}{138}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Chaleur molaire}{142}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Chaleur molaire}{138}\protected@file@percent }
|
||||||
\newlabel{chaleurmolaire}{{11.7}{142}}
|
\newlabel{chaleurmolaire}{{11.7}{138}}
|
||||||
\newlabel{Qchaleurmolaire}{{11.8}{143}}
|
\newlabel{Qchaleurmolaire}{{11.8}{139}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Relation entre chaleur massique et molaire}{143}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Relation entre chaleur massique et molaire}{139}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Chaleur latente}{143}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Chaleur latente}{139}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.4}{\ignorespaces Chaleur latente\relax }}{143}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.4}{\ignorespaces Chaleur latente\relax }}{139}\protected@file@percent }
|
||||||
\newlabel{chaleurlatente}{{11.4}{143}}
|
\newlabel{chaleurlatente}{{11.4}{139}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}vaporation}{144}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}vaporation}{140}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.3}Bilan thermique}{144}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.2.3}Bilan thermique}{140}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.3}Loi des gaz parfaits}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.3}Loi des gaz parfaits}{141}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.3.1}\IeC {\'E}quation d'\IeC {\'e}tat}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.3.1}\IeC {\'E}quation d'\IeC {\'e}tat}{141}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Pression}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Pression}{141}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}tat d'un gaz parfait}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}tat d'un gaz parfait}{141}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Approche intuitive}{145}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Approche intuitive}{141}\protected@file@percent }
|
||||||
\newlabel{pvkt}{{11.12}{146}}
|
\newlabel{pvkt}{{11.12}{142}}
|
||||||
\newlabel{nRNk}{{11.14}{146}}
|
\newlabel{nRNk}{{11.14}{142}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Approche mol\IeC {\'e}culaire}{146}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Approche mol\IeC {\'e}culaire}{142}\protected@file@percent }
|
||||||
\newlabel{apprmolecul}{{11.3.1}{146}}
|
\newlabel{apprmolecul}{{11.3.1}{142}}
|
||||||
\newlabel{tempencin}{{11.19}{147}}
|
\newlabel{tempencin}{{11.19}{143}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.3.2}Gaz parfait}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.3.2}Gaz parfait}{143}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.4}Premier principe}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.4}Premier principe}{143}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.1}Chaleur}{147}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.1}Chaleur}{143}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.2}Travail}{148}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.2}Travail}{144}\protected@file@percent }
|
||||||
\newlabel{generaltravail}{{11.20}{148}}
|
\newlabel{generaltravail}{{11.20}{144}}
|
||||||
\newlabel{generalpression}{{11.21}{148}}
|
\newlabel{generalpression}{{11.21}{144}}
|
||||||
\newlabel{thermotravail}{{11.22}{148}}
|
\newlabel{thermotravail}{{11.22}{144}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.4}{\ignorespaces Travail et diagramme P-V\relax }}{148}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.4}{\ignorespaces Travail et diagramme P-V\relax }}{144}\protected@file@percent }
|
||||||
\newlabel{diagtravailpv}{{11.4}{148}}
|
\newlabel{diagtravailpv}{{11.4}{144}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.3}\IeC {\'E}nergie interne}{148}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.3}\IeC {\'E}nergie interne}{144}\protected@file@percent }
|
||||||
\newlabel{eninterne}{{11.23}{148}}
|
\newlabel{eninterne}{{11.23}{144}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}quipartition de l'\IeC {\'e}nergie}{149}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{\IeC {\'E}quipartition de l'\IeC {\'e}nergie}{145}\protected@file@percent }
|
||||||
\newlabel{equipartition}{{11.24}{149}}
|
\newlabel{equipartition}{{11.24}{145}}
|
||||||
\newlabel{iequipartition}{{11.25}{149}}
|
\newlabel{iequipartition}{{11.25}{145}}
|
||||||
\newlabel{iequipartitiondiatomique}{{11.26}{149}}
|
\newlabel{iequipartitiondiatomique}{{11.26}{145}}
|
||||||
\newlabel{iequipartitiondiatomiquevibrant}{{11.27}{149}}
|
\newlabel{iequipartitiondiatomiquevibrant}{{11.27}{145}}
|
||||||
\newlabel{iequipartitiontriatomique}{{11.28}{149}}
|
\newlabel{iequipartitiontriatomique}{{11.28}{145}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.4}Premier principe}{149}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.4}Premier principe}{145}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.5}Changements d'\IeC {\'e}tats}{149}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.5}Changements d'\IeC {\'e}tats}{145}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Transformation isobare}{150}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Transformation isobare}{146}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.5}{\ignorespaces Transformation isobare\relax }}{150}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.5}{\ignorespaces Transformation isobare\relax }}{146}\protected@file@percent }
|
||||||
\newlabel{diagtravailpvisobare}{{11.5}{150}}
|
\newlabel{diagtravailpvisobare}{{11.5}{146}}
|
||||||
\newlabel{chaleurspecisobare}{{11.33}{150}}
|
\newlabel{chaleurspecisobare}{{11.33}{146}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Transformation isochore}{150}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Transformation isochore}{146}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.6}{\ignorespaces Transformation isochore\relax }}{151}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.6}{\ignorespaces Transformation isochore\relax }}{147}\protected@file@percent }
|
||||||
\newlabel{diagtravailpvisochore}{{11.6}{151}}
|
\newlabel{diagtravailpvisochore}{{11.6}{147}}
|
||||||
\newlabel{enintisochore}{{11.35}{151}}
|
\newlabel{enintisochore}{{11.35}{147}}
|
||||||
\newlabel{chaleurspecisochore}{{11.37}{151}}
|
\newlabel{chaleurspecisochore}{{11.37}{147}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Transformation isotherme}{151}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Transformation isotherme}{147}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.7}{\ignorespaces Transformation isotherme\relax }}{151}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.7}{\ignorespaces Transformation isotherme\relax }}{147}\protected@file@percent }
|
||||||
\newlabel{diagtravailpvisotherme}{{11.7}{151}}
|
\newlabel{diagtravailpvisotherme}{{11.7}{147}}
|
||||||
\newlabel{travailisotherme}{{11.40}{151}}
|
\newlabel{travailisotherme}{{11.40}{147}}
|
||||||
\@writefile{toc}{\contentsline {subsubsection}{Transformation adiabatique}{152}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsubsection}{Transformation adiabatique}{148}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.8}{\ignorespaces Transformation adiabatique\relax }}{152}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.8}{\ignorespaces Transformation adiabatique\relax }}{148}\protected@file@percent }
|
||||||
\newlabel{diagtravailpvadiabatique}{{11.8}{152}}
|
\newlabel{diagtravailpvadiabatique}{{11.8}{148}}
|
||||||
\newlabel{adiabaU0}{{11.41}{152}}
|
\newlabel{adiabaU0}{{11.41}{148}}
|
||||||
\newlabel{adiabaU}{{11.42}{152}}
|
\newlabel{adiabaU}{{11.42}{148}}
|
||||||
\newlabel{adiabdiff}{{11.43}{152}}
|
\newlabel{adiabdiff}{{11.43}{148}}
|
||||||
\newlabel{adiabadef}{{11.44}{152}}
|
\newlabel{adiabadef}{{11.44}{148}}
|
||||||
\newlabel{equationadiabatique}{{11.46}{152}}
|
\newlabel{equationadiabatique}{{11.46}{148}}
|
||||||
\newlabel{adiavariation1}{{11.47}{152}}
|
\newlabel{adiavariation1}{{11.47}{148}}
|
||||||
\newlabel{adiavariation2}{{11.48}{153}}
|
\newlabel{adiavariation2}{{11.48}{149}}
|
||||||
\newlabel{travailadiabatique}{{11.49}{153}}
|
\newlabel{travailadiabatique}{{11.49}{149}}
|
||||||
\newlabel{gammacpcv}{{11.50}{153}}
|
\newlabel{gammacpcv}{{11.50}{149}}
|
||||||
\newlabel{tvadiabat}{{11.57}{153}}
|
\newlabel{tvadiabat}{{11.57}{149}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.6}Chaleurs sp\IeC {\'e}cifiques}{153}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.4.6}Chaleurs sp\IeC {\'e}cifiques}{149}\protected@file@percent }
|
||||||
\newlabel{cpi}{{11.60}{153}}
|
\newlabel{cpi}{{11.60}{149}}
|
||||||
\newlabel{cvi}{{11.61}{153}}
|
\newlabel{cvi}{{11.61}{149}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.5}Machines thermiques}{154}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.5}Machines thermiques}{150}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.1}Machine simple}{154}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.1}Machine simple}{150}\protected@file@percent }
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.5}{\ignorespaces \IeC {\'E}tats caract\IeC {\'e}ristiques\relax }}{154}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.5}{\ignorespaces \IeC {\'E}tats caract\IeC {\'e}ristiques\relax }}{150}\protected@file@percent }
|
||||||
\newlabel{etats}{{11.5}{154}}
|
\newlabel{etats}{{11.5}{150}}
|
||||||
\newlabel{moteur1}{{11.9(a)}{155}}
|
\newlabel{moteur1}{{11.9(a)}{151}}
|
||||||
\newlabel{sub@moteur1}{{(a)}{155}}
|
\newlabel{sub@moteur1}{{(a)}{151}}
|
||||||
\newlabel{moteur2}{{11.9(b)}{155}}
|
\newlabel{moteur2}{{11.9(b)}{151}}
|
||||||
\newlabel{sub@moteur2}{{(b)}{155}}
|
\newlabel{sub@moteur2}{{(b)}{151}}
|
||||||
\newlabel{moteur3}{{11.9(c)}{155}}
|
\newlabel{moteur3}{{11.9(c)}{151}}
|
||||||
\newlabel{sub@moteur3}{{(c)}{155}}
|
\newlabel{sub@moteur3}{{(c)}{151}}
|
||||||
\newlabel{moteur4}{{11.9(d)}{155}}
|
\newlabel{moteur4}{{11.9(d)}{151}}
|
||||||
\newlabel{sub@moteur4}{{(d)}{155}}
|
\newlabel{sub@moteur4}{{(d)}{151}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.9}{\ignorespaces Moteur thermique}}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.9}{\ignorespaces Moteur thermique}}{151}\protected@file@percent }
|
||||||
\newlabel{moteurtherm}{{11.9}{155}}
|
\newlabel{moteurtherm}{{11.9}{151}}
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Chargement}}}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Chargement}}}{151}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Chauffage}}}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Chauffage}}}{151}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {D\IeC {\'e}chargement}}}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {D\IeC {\'e}chargement}}}{151}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(d)}{\ignorespaces {Refroidissement}}}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(d)}{\ignorespaces {Refroidissement}}}{151}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.10}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{155}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.10}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{151}\protected@file@percent }
|
||||||
\newlabel{diagpvmotsimple}{{11.10}{155}}
|
\newlabel{diagpvmotsimple}{{11.10}{151}}
|
||||||
\@writefile{lot}{\contentsline {table}{\numberline {11.6}{\ignorespaces Grandeurs caract\IeC {\'e}ristiques\relax }}{156}\protected@file@percent }
|
\@writefile{lot}{\contentsline {table}{\numberline {11.6}{\ignorespaces Grandeurs caract\IeC {\'e}ristiques\relax }}{152}\protected@file@percent }
|
||||||
\newlabel{transetats}{{11.6}{156}}
|
\newlabel{transetats}{{11.6}{152}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.11}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{156}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.11}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{152}\protected@file@percent }
|
||||||
\newlabel{diagpvchal}{{11.11}{156}}
|
\newlabel{diagpvchal}{{11.11}{152}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.12}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{156}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.12}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{152}\protected@file@percent }
|
||||||
\newlabel{bilanmot}{{11.12}{156}}
|
\newlabel{bilanmot}{{11.12}{152}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.2}Moteur \IeC {\`a} explosion}{156}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.2}Moteur \IeC {\`a} explosion}{152}\protected@file@percent }
|
||||||
\newlabel{paraOtto}{{11.5.2}{156}}
|
\newlabel{paraOtto}{{11.5.2}{152}}
|
||||||
\newlabel{admission}{{11.13(a)}{157}}
|
\newlabel{admission}{{11.13(a)}{153}}
|
||||||
\newlabel{sub@admission}{{(a)}{157}}
|
\newlabel{sub@admission}{{(a)}{153}}
|
||||||
\newlabel{compression}{{11.13(b)}{157}}
|
\newlabel{compression}{{11.13(b)}{153}}
|
||||||
\newlabel{sub@compression}{{(b)}{157}}
|
\newlabel{sub@compression}{{(b)}{153}}
|
||||||
\newlabel{allumage}{{11.13(c)}{157}}
|
\newlabel{allumage}{{11.13(c)}{153}}
|
||||||
\newlabel{sub@allumage}{{(c)}{157}}
|
\newlabel{sub@allumage}{{(c)}{153}}
|
||||||
\newlabel{tempsmoteur}{{11.13(d)}{157}}
|
\newlabel{tempsmoteur}{{11.13(d)}{153}}
|
||||||
\newlabel{sub@tempsmoteur}{{(d)}{157}}
|
\newlabel{sub@tempsmoteur}{{(d)}{153}}
|
||||||
\newlabel{echappement}{{11.13(e)}{157}}
|
\newlabel{echappement}{{11.13(e)}{153}}
|
||||||
\newlabel{sub@echappement}{{(e)}{157}}
|
\newlabel{sub@echappement}{{(e)}{153}}
|
||||||
\newlabel{evacuation}{{11.13(f)}{157}}
|
\newlabel{evacuation}{{11.13(f)}{153}}
|
||||||
\newlabel{sub@evacuation}{{(f)}{157}}
|
\newlabel{sub@evacuation}{{(f)}{153}}
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.13}{\ignorespaces Moteur \IeC {\`a} explosion}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.13}{\ignorespaces Moteur \IeC {\`a} explosion}}{153}\protected@file@percent }
|
||||||
\newlabel{motess}{{11.13}{157}}
|
\newlabel{motess}{{11.13}{153}}
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Admission}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(a)}{\ignorespaces {Admission}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Compression}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(b)}{\ignorespaces {Compression}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {Allumage}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(c)}{\ignorespaces {Allumage}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(d)}{\ignorespaces {Temps moteur}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(d)}{\ignorespaces {Temps moteur}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(e)}{\ignorespaces {\IeC {\'E}chappement}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(e)}{\ignorespaces {\IeC {\'E}chappement}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {subfigure}{\numberline{(f)}{\ignorespaces {\IeC {\'E}vacuation}}}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {subfigure}{\numberline{(f)}{\ignorespaces {\IeC {\'E}vacuation}}}{153}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.14}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{157}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.14}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{153}\protected@file@percent }
|
||||||
\newlabel{diagetatmotess}{{11.14}{157}}
|
\newlabel{diagetatmotess}{{11.14}{153}}
|
||||||
\newlabel{rendementotto}{{11.64}{158}}
|
\newlabel{rendementotto}{{11.64}{154}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.3}Moteur Diesel}{158}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.3}Moteur Diesel}{154}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.15}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{158}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.15}{\ignorespaces Diagramme d'\IeC {\'e}tat\relax }}{154}\protected@file@percent }
|
||||||
\newlabel{diagetatmotdiesel}{{11.15}{158}}
|
\newlabel{diagetatmotdiesel}{{11.15}{154}}
|
||||||
\newlabel{T3T2V3V2}{{11.65}{159}}
|
\newlabel{T3T2V3V2}{{11.65}{155}}
|
||||||
\newlabel{eqqq1}{{11.66}{159}}
|
\newlabel{eqqq1}{{11.66}{155}}
|
||||||
\newlabel{eqqq2}{{11.67}{159}}
|
\newlabel{eqqq2}{{11.67}{155}}
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.4}Machine de Stirling}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.4}Machine de Stirling}{156}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.5}Climatiseur}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.5}Climatiseur}{156}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.6}R\IeC {\'e}frig\IeC {\'e}rateur}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.6}R\IeC {\'e}frig\IeC {\'e}rateur}{156}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.7}Pompe \IeC {\`a} chaleur}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.7}Pompe \IeC {\`a} chaleur}{156}\protected@file@percent }
|
||||||
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.8}Cycle de Carnot}{160}\protected@file@percent }
|
\@writefile{toc}{\contentsline {subsection}{\numberline {11.5.8}Cycle de Carnot}{156}\protected@file@percent }
|
||||||
\@writefile{lof}{\contentsline {figure}{\numberline {11.16}{\ignorespaces Le cycle de Carnot\relax }}{160}\protected@file@percent }
|
\@writefile{lof}{\contentsline {figure}{\numberline {11.16}{\ignorespaces Le cycle de Carnot\relax }}{156}\protected@file@percent }
|
||||||
\newlabel{diagpvcarnot}{{11.16}{160}}
|
\newlabel{diagpvcarnot}{{11.16}{156}}
|
||||||
\newlabel{rendementcarnot}{{11.68}{161}}
|
\newlabel{rendementcarnot}{{11.68}{157}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.6}Thermodynamique statistique}{161}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.6}Thermodynamique statistique}{157}\protected@file@percent }
|
||||||
\newlabel{thermostat}{{11.6}{161}}
|
\newlabel{thermostat}{{11.6}{157}}
|
||||||
\newlabel{entropie}{{11.69}{161}}
|
\newlabel{entropie}{{11.69}{157}}
|
||||||
\@writefile{toc}{\contentsline {section}{\numberline {11.7}Second principe}{162}\protected@file@percent }
|
\@writefile{toc}{\contentsline {section}{\numberline {11.7}Second principe}{158}\protected@file@percent }
|
||||||
\newlabel{secondprincipe}{{11.7}{162}}
|
\newlabel{secondprincipe}{{11.7}{158}}
|
||||||
\@setckpt{ThermodynamiqueOS/ThermodynamiqueOS}{
|
\@setckpt{ThermodynamiqueOS/ThermodynamiqueOS}{
|
||||||
\setcounter{page}{163}
|
\setcounter{page}{159}
|
||||||
\setcounter{equation}{69}
|
\setcounter{equation}{69}
|
||||||
\setcounter{enumi}{3}
|
\setcounter{enumi}{3}
|
||||||
\setcounter{enumii}{0}
|
\setcounter{enumii}{0}
|
||||||
|
|||||||
Loading…
Reference in New Issue
Block a user