Correction d'un signe et du diagramme p-V du moteur diesel
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[]\T1/lmr/m/n/10 Le gaz est chauffé par une
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[160]
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[]\T1/lmr/bx/n/14.4 Thermodynamique sta-
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[]
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Before Width: | Height: | Size: 18 KiB After Width: | Height: | Size: 20 KiB |
File diff suppressed because it is too large
Load Diff
@ -1230,6 +1230,9 @@ Le fonctionnement d'un moteur diésel n'est pas très différent de celui d'un m
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\psfrag{A}{\(A\)}
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@ -1243,7 +1246,7 @@ Comme le cycle d'Otto, le cycle Diesel est donc aussi constitué de deux adiabat
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\[Q_{abs}=n\cdot C_P\cdot (T_3-T_2)\]
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et, comme chaleur rejetée~:
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\[Q_{rej}=n\cdot C_V\cdot (T_1-T_4)\]
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La différence constitue le travail fourni par le système pendant le cycle, une partie étant produite par le gaz pendant le temps moteur et une autre absorbée par celui-ci pendant la compression. Attention, \(Q_{rej}>0\) et il faut donc soit additionner les deux chaleur pour avoir le travail qui constitue leur différence ou soustraire l'opposé de la chaleur rejetée, soit \(|Q_{rej}|=n\cdot C_V\cdot (T_4-T_1)\). On a donc~:
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La différence constitue le travail fourni par le système pendant le cycle, une partie étant produite par le gaz pendant le temps moteur et une autre absorbée par celui-ci pendant la compression. Attention, \(Q_{rej}<0\) et il faut donc soit additionner les deux chaleur pour avoir le travail qui constitue leur différence ou soustraire l'opposé de la chaleur rejetée, soit \(|Q_{rej}|=n\cdot C_V\cdot (T_4-T_1)\). On a donc~:
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\begin{align*}
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A&=Q_{abs}-Q_{rej}\\
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&=n\cdot C_P\cdot (T_3-T_2)-n\cdot C_V\cdot (T_4-T_1)
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||||
Loading…
Reference in New Issue
Block a user