Solve Asymmetric Piston Problem for SL

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Greetings!

Can you help me understand what this text book problem asks of me?
piston.PNG


The situation was considered in the text: In equilibrium, the forces on both sides of the piston are equal: ##A_1P_1 = A_2P_2##.
This is the first equation. It should also answer part 3 of the question. The piston allows heat exchange, so that in equilibrium I have ##T_1=T_2##. This should answer part 2. To get a second equation to answer part one, I can just apply the ideal gas law to the first equation to get
$$
A_j\frac{N_j}{V_j} = A_k\frac{N_k}{V_k}.
$$

I feel like this is way too easy and I am missing something... I don't know what the author wants me to do. I should note that he derived the entropy function S(E,V,N) of the ideal gas, and also the three partial derivatives such as ##\left(\frac{\partial S}{\partial V}\right)_{E,N}=\frac {P} {T} ##, so maybe he expects some more wizardry with them?SL
 
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on Phys.org
The problem says the piston is diathermal so ##T_1 \neq T_2##.

EDIT I confused it with adiabatic.
 
Last edited:
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anuttarasammyak said:
The problem says the piston is diathermal so ##T_1 \neq T_2##.
Diathermal means that the temperature ARE equal in the end.
 
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I don't know what the author had in mind, but here are some thoughts on how I would approach this problem (assuming the same gas species is in both chambers). For the final temperature, I would have $$T=\frac{(E_1+E_2)}{C_v(N_1+N_2)}$$
For the final volumes, I would have: $$V_1=V_{10}+A_1\delta$$$$V_2=V_{20}-A_2\delta$$where ##\delta## is the displacement of the piston. So, for the final pressures, we would have: $$P_1=\frac{N_1RT}{V_1}$$$$P_2=\frac{N_2RT}{V_2}$$subject to $$P_1A_1=P_2A_2$$This provides sufficient information to determine the piston displacement ##\delta##.
 
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Thanks Chestermiller!

The author did not ask for the displacement, so it is really unclear what he even expects. Glad to know that I did not miss something obvious.
 
To get the final pressure, you need to first solve for the displacement.
 

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