Heat Transfer in Ideal Gases: An Example of Path Dependence

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Homework Help Overview

The discussion revolves around the concept of heat transfer in ideal gases, specifically focusing on the path dependence of heat during thermodynamic processes. Participants explore scenarios involving two different gases in a container transitioning from an adiabatic to a diathermic wall, examining how changes in pressure and volume affect the heat transfer involved.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss different paths taken to reach the same thermodynamic state, questioning the implications of these paths on heat transfer. They raise inquiries about the nature of path dependence and seek clarification on when heat transfer is path independent versus path dependent.

Discussion Status

The discussion is ongoing, with participants expressing confusion about the implications of path dependence in heat transfer. Some guidance has been offered regarding the differences in processes, but there is no explicit consensus on the underlying principles or calculations involved.

Contextual Notes

Participants are working under the constraints of ideal gas behavior and are considering specific processes (isochoric and isobaric) while discussing the implications of these processes on heat transfer. There is an emphasis on understanding the first law of thermodynamics and the conditions of the system.

hiba fatima
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< Mentor Note -- Posts split off from an old thread to preserve very good helpful responses...>[/color]

how is heat path dependent?prove with an example?
 
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gerardpc said:
I've read a solution of a problem, in which there are two different gases in a container, initally at equilibrium and separated by an adiabatic fix wall. At some time, this wall is changed by a diathermic mobile wall, so the equilibrium point changes. You have to find the final state of the gases, given the initial volumes, temperatures and pressions.

Then the solution says: we will divide the process in two parts: first an isochoric process and after that and isothermal one. But it is clear that pressure and temperature evolve at the same time.
I'm making a bit of a mess here: is it path dependent or indpendent? In a generic process, when is it path independent and when it is not? And why?
Consider an ideal gas at initial state (p1,V1,T1). We want to change the state to (p2,V2,T2).

We can do this in many ways, but let's pick two in particular :
1. we can change the temperature at constant V1 (isochoric) until p = p2, then, holding p constant, change the temperature some more until V = V2. We have reached (p2,V2,T2).
2. we can change the temperature at constant p1 (isobaric) until V = V2, then, holding V constant, change temperature some more until p = p2. We have again reached (p2,V2,T2).
In both cases we went from state (p1,V1,T1) to (p2,V2,T2).
Can you compute the heat and work required in both processes?
 
thanx ... but you did not clear the point that the heat is path dependent...means we go to the same state in both cases...but what is the difference in both cases that makes the heat path dependent...
 
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hiba fatima said:
thanx ... bt u did not clear the point that the heat is path dependent...means we go to the same state in both cases...but what is the difference in both cases that makes the heat path dependent...
The difference is in one case we change p first and then V, in the other we change V first and then p. The sequence makes it different. Compute W and Q for both cases and you will see.
 
i could not do it :(
 
hiba fatima said:
i could not do it :(
What is the area under a p-V curve going from a state 1 to a state 2?
 
I assume you are dealing with ideal gases. If the gases are in a rigid container, how much external work do the combination of gases do on the surroundings? Assuming that the container is adiabatic, how much heat passes through the walls of the container. From the first law of thermodynamics, what is the change in internal energy for the combination of gases when the system finally equilibrates? If the wall is mobile and diathermal, how do the temperatures and pressures in the two compartments compare at the final equilibrium state?

Chet
 

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