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reversible adiabatic expansion |
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| Apr15-10, 02:31 PM | #1 |
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reversible adiabatic expansion
1. The problem statement, all variables and given/known data
I'm in a rutt for a tutorial question: The question is basically to show that the work done during a reversible adiabatic expansion of an ideal gas is W = (P1V1 – P2V2)/(1 ‐ γ) ........ Y is gamma 2. Relevant equations 3. The attempt at a solution I've got so far as to get W= (P1V1^γ – P2V2^γ) due to P1V1^γ being constant for a reversible adiabat also that W= -PdV But i havent a clue how to get the 1-Y at the bottom, me thinks its intergrating for V to get this but my maths is very bad so i dont know how to do this. |
| Apr15-10, 08:55 PM | #2 |
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If [tex]PV^\gamma[/tex] is a constant, then finding the difference in it would be 0, and not equal to the work. For more help on this, please check the wikipedia page:
http://en.wikipedia.org/wiki/Adiabatic_process |
| Apr16-10, 12:05 PM | #3 |
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Recognitions:
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Since [itex]\Delta Q = 0[/itex] and [itex]\Delta U = nC_v\Delta T[/itex] where [itex]C_v = R/(\gamma - 1)[/itex] you should be able to work it out quickly. (Hint: apply the ideal gas law: PV=nRT). AM |
| Apr16-10, 01:33 PM | #4 |
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reversible adiabatic expansion
still lost
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| Apr16-10, 03:59 PM | #5 |
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Recognitions:
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(1) [tex]\therefore W = - \Delta U[/tex] Now: (2) [tex]\Delta U = nC_v\Delta T[/tex] and [tex]C_v = C_p/\gamma = (C_v+R)/\gamma[/tex] so: (3) [tex]C_v = R/(\gamma-1)[/tex] Substitute (3) into (2) and then just substitute PV for nRT AM |
| Apr17-10, 03:27 AM | #6 |
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Cheers, i got it
The way you showed was much easier then the way i was going about it |
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| adiabatic expansion, thermodynamic |
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