Thermal equilibrium - Entropy driven

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SUMMARY

The discussion revolves around a statistical mechanics problem involving thermal equilibrium in a chamber divided into two sections, one filled with an ideal gas at temperature T0 and the other empty. The final temperature of the system is determined by maximizing entropy, as thermal equilibrium is achieved. For the Van der Waals gas, the equation \(\left(p + \frac{n^2 a}{V^2}\right)\left(V-nb\right) = nRT\) is suggested for analysis, highlighting the differences in behavior compared to an ideal gas. The first law of thermodynamics is also emphasized to analyze changes in internal energy and temperature.

PREREQUISITES
  • Understanding of statistical mechanics principles
  • Familiarity with the ideal gas law (PV = nRT)
  • Knowledge of Van der Waals equation for real gases
  • Basic concepts of thermodynamics, particularly the first law
NEXT STEPS
  • Explore the implications of entropy maximization in thermodynamic systems
  • Study the differences between ideal gases and Van der Waals gases
  • Investigate the first law of thermodynamics and its applications in gas systems
  • Learn about the concept of thermal equilibrium and its significance in statistical mechanics
USEFUL FOR

Students and educators in physics, particularly those focusing on thermodynamics and statistical mechanics, as well as researchers interested in gas behavior under varying conditions.

Stiibe
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Hey there. We are struggling with a problem from an old exam about statistical mechanics. I hope you can help us or give any clues. Here is the problem.

Homework Statement



A chamber is divided by a wall into two sections of equal volume. One section of the chamber is initially filled by an ideal gas at temperature T0, whereas the other section is empty. Then, a small hole is opened in the dividing wall such that the gas can flow through, until equilibrium is reached. Consider the chamber isolated towards the surrounding and no heat is exchanged with the walls.

a) What is the final Temperature of the system?b)How does the result change if instead initially the chamber is filled with a Van der Waals gas?

Homework Equations



Any thermodynamical equation.

The Attempt at a Solution



We tried to solve the problem by using the entropy. Since thermal equilibrium is reached, wehn the entropy is maximized.
 
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Stiibe said:
Hey there. We are struggling with a problem from an old exam about statistical mechanics. I hope you can help us or give any clues. Here is the problem.

Homework Statement



A chamber is divided by a wall into two sections of equal volume. One section of the chamber is initially filled by an ideal gas at temperature T0, whereas the other section is empty. Then, a small hole is opened in the dividing wall such that the gas can flow through, until equilibrium is reached. Consider the chamber isolated towards the surrounding and no heat is exchanged with the walls.

a) What is the final Temperature of the system?


b)How does the result change if instead initially the chamber is filled with a Van der Waals gas?


Homework Equations



Any thermodynamical equation.

The Attempt at a Solution



We tried to solve the problem by using the entropy. Since thermal equilibrium is reached, wehn the entropy is maximized.
The first equation that crosses my mind for part a) is the famous PV=NRT.
For part b), wikipedia tells us \left(p + \frac{n^2 a}{V^2}\right)\left(V-nb\right) = nRT. So I suggest you to use these 2 equations rather than the entropy.
 
Stiibe said:
Hey there. We are struggling with a problem from an old exam about statistical mechanics. I hope you can help us or give any clues. Here is the problem.

Homework Statement



A chamber is divided by a wall into two sections of equal volume. One section of the chamber is initially filled by an ideal gas at temperature T0, whereas the other section is empty. Then, a small hole is opened in the dividing wall such that the gas can flow through, until equilibrium is reached. Consider the chamber isolated towards the surrounding and no heat is exchanged with the walls.

a) What is the final Temperature of the system?
Does the gas do any work? When you answer that question, apply the first law to determine the change in internal energy. What does that tell you about the change in temperature?

b)How does the result change if instead initially the chamber is filled with a Van der Waals gas?
Apply the same first law analysis. In this case, however, how is temperature related to volume and internal energy in a Van der Waals gas? (Hint: in an ideal gas, the temperature is a function of internal energy and independent of volume. Does the same apply to a Van der Waals gas?)

AM
 

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