Solve Thermal Equilibrium Homework Problem

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SUMMARY

The discussion focuses on solving a thermal equilibrium problem involving two objects, A and B, each containing N molecules. The entropies are defined as S_A = Nkln(U_A/N) and S_B = (3/2)Nkln(U_B/N). The key to finding the final temperature is applying the equation 1/T = ∂S/∂U and ensuring that the change in entropy is equal for both objects at equilibrium. The approach involves calculating the change in internal energy (ΔU) and subsequently determining the final temperature.

PREREQUISITES
  • Understanding of thermodynamic concepts, specifically entropy and internal energy.
  • Familiarity with the mathematical derivation of thermodynamic equations.
  • Knowledge of partial derivatives in the context of thermodynamics.
  • Basic principles of statistical mechanics related to molecular systems.
NEXT STEPS
  • Study the derivation of the entropy formula for ideal gases.
  • Learn about the implications of the first law of thermodynamics in thermal equilibrium.
  • Explore the concept of heat transfer and its relation to changes in internal energy.
  • Investigate the application of partial derivatives in thermodynamic equations.
USEFUL FOR

Students and professionals in physics, particularly those studying thermodynamics and statistical mechanics, will benefit from this discussion. It is also relevant for anyone tackling thermal equilibrium problems in their coursework or research.

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Homework Statement


Two objects A and B, with an equal number, N, of molecules are brought into thermal contact. The first has entropy [tex]S_A = Nkln(U_A/N)[/tex] and the second has entropy [tex]S_B = 3/2 * Nkln(U_B/N)[/tex]. What is the final temperature?

Homework Equations


[tex]\frac{1}{T} = \frac{\partial S}{\partial U}[/tex]


The Attempt at a Solution


My process would be to take
[tex]\frac{\partial}{\partial U}Nkln((U_A + \Delta U) / N) = \frac{\partial}{\partial U}3/2 * Nkln((U_b - \Delta U)/N)[/tex]

And solve for delta U. Is this the best way to approach the problem?
 
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I think your way is mostly right. As you said, the criteria at equilibrium is,

[tex]\left( \frac{\partial S}{\partial U} \right) |_{U_A + \Delta U} = \left( \frac{\partial S}{\partial U} \right) |_{U_A - \Delta U}[/tex]

Find [itex]\Delta U[/itex], and from that, the final temperature.
 

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