Two gases in a cylinder separated by an insulating piston.

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Homework Help Overview

The problem involves a cylinder divided into two chambers by a frictionless, insulating piston, with each chamber containing helium gas at different initial pressures. The goal is to analyze the behavior of the system as the piston moves to equalize pressures after being allowed to slide freely.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss identifying the type of thermodynamic process occurring (e.g., adiabatic) and question the implications of insulation on heat transfer.
  • Some participants suggest calculating initial temperatures and work done by the gas, while others emphasize the importance of understanding the system's energy changes and equilibrium states.
  • There is a focus on the relationship between pressure, volume, and temperature in the context of ideal gases and the implications of the piston's movement.

Discussion Status

The discussion is active, with participants exploring various interpretations of the problem. Some have offered insights into the relationships between pressure, volume, and temperature, while others are questioning assumptions about the nature of the process and the role of the piston. There is no explicit consensus yet, but several productive lines of reasoning are being developed.

Contextual Notes

Participants note that the problem involves ideal gases and that the system is insulated, which affects heat transfer considerations. There is also mention of the potential impact of the piston's mass on the process being quasi-static.

Tiberius47
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Homework Statement


A cylinder of cross-sectional area A is divided into two chambers 1 and 2, by means of a frictionless piston. The piston as well as the walls of the chambers are heat-insulating, and the chambers initially have equal length L. Both chambers are filled with 1 mol of helium gas, with initial pressures 2Po and Po, respectively. The pisotn is then allowed to slide freely, whereupon the gas in chamber 1 pushes the piston a distance a to equalize the pressures to P.
(a) Find the distance a traveled by the piston.
(b) If W is the work done by the gas chamber 1, what are the final temperatures T1 and T2 in the two chambers? What is the final pressure P?
(c) Find W, the work done.

Homework Equations



PV=NRT

The Attempt at a Solution



I know that the pressures will be equal at equilibrium but I'm not sure how to set up the problem.
 
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To tackle this problem, I believe you first need to identify what kind of process is taking place (isobaric, isothermal, isochoric, adiabatic, etc). Which process do you think this is?
 
Mute said:
To tackle this problem, I believe you first need to identify what kind of process is taking place (isobaric, isothermal, isochoric, adiabatic, etc). Which process do you think this is?

Well given that the two chambers are insulated I would say adiabatic. So the change in heat would be zero so:

ΔU+W=0
 
Last edited:
Tiberius47 said:
Well given that the two chambers are insulated I would say adiabatic. So the change in heat would be zero so:

ΔU+W=0

Since mute is not on the air -
yes, adiabatic. So what p-v relationship can you ascribe to each half?
 
This is a very interesting and "meaty" problem. The first thing to do is to calculate the initial temperatures in each of the two chambers in terms of p0, V0=AL, and R. What are your results for this? The next step is to skip part (a) and most of part (b), and determine the final pressure p. To do this, you should first answer the question "How much work is done by the combined system in the two chambers?" Once you answer this question, you will be able to ascertain the answer to the question "What is the change in internal energy for the combined system?" Once you know the answer to this question, you should be able to answer the question "How is the sum of temperatures in the two chambers in the final equilibrium state related to the sum of the temperatures in the two chambers prior to release of the piston?" Next, express the volume of each chamber algebraically in terms of its temperature and pressure in the final state. Next, what is the sum of the two chamber volumes in the final state? Express this algebraically in terms of the temperatures and the pressure in the final state, and recognize that the algebraic expression involves the sum of the temperatures. Solve for the pressure.
Of course, this all is just the first step in the solution to the problem as posed. But, it gives you a good start.
 
Not necessary to solve for initial temperatures. 3 equations yield final pressure and both final volumes. Thus arriving at final temperatures. Then the 1st law gets us W.

I am assuming ideal gases.

EDIT: oops, we do too need the initial temperatures, but just to find W.
 
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rude man said:
Not necessary to solve for initial temperatures. 3 equations yield final pressure and both final volumes. Thus arriving at final temperatures. Then the 1st law gets us W.

I am assuming ideal gases.

Are you assuming that pVγ= constant? That is correct if the piston is forced to move slowly, but if the piston is free to slide (as specified in the problem statement), that is not the correct relationship to use. Better be very careful.

Chet
 
Chestermiller said:
Are you assuming that pVγ= constant? That is correct if the piston is forced to move slowly, but if the piston is free to slide (as specified in the problem statement), that is not the correct relationship to use. Better be very careful.

Chet

I understand that that relationship does not hold for the nonequilibrium states in transitioning from the initial to the final state, but I did think it applied to the initial and final equilibrium states.

I can't wait to see this thread through ...
 
rude man said:
I understand that that relationship does not hold for the nonequilibrium states in transitioning from the initial to the final state, but I did think it applied to the initial and final equilibrium states.

Actually, no. If you consider the combination of the two chambers and the piston as your system, then the system does no work on the surroundings. Therefore, since no heat enters or leaves the system, the change in internal energy of the system between the initial and final equilibrium states is zero. This means that, for an ideal gas, the sum of the temperatures in the two chambers is the same in the final equilibrium state as in the initial equilibrium state. This gives you enough information to calculate the final equilibrium pressure of the system. Of course, because of the fact that the piston is insulated, the final temperatures in the two chambers will not be equal.
 
  • #10
Thanks for the revelation, Chester. But what if the piston were sufficiently massive to effect a quasi-static transformation - there would admittedly be kinetic energy of the piston to consider, but the beginning and end k.e.'s would both be zero?

EDIT: I guess thre would be no change in the system. The only way to effect a quasi-static process here is to allow the higher-pressure gas to apply work externally, right?
 
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  • #11
rude man said:
Thanks for the revelation, Chester. But what if the piston were sufficiently massive to effect a quasi-static transformation - there would admittedly be kinetic energy of the piston to consider, but the beginning and end k.e.'s would both be zero?

EDIT: I guess thre would be no change in the system. The only way to effect a quasi-static process here is to allow the higher-pressure gas to apply work externally, right?

Yes. You're right. The piston ke would be zero at the beginning and end, so it would have no effect on the final equilibrium state.

Actually, if you did it quasi-staticaly, by,say, attaching a rod to the piston, you would have to take into account both the high pressure and the low pressure chamber pressures, and the work on the surroundings would be the difference between the two pressures integrated over the change in volume of one of the chambers.
 

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