Thermodynamics: Entropy of 2 large Einstein Solids

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Homework Help Overview

The discussion revolves around the entropy of a system consisting of two large, identical Einstein solids, each with a significant number of oscillators. The problem involves calculating entropy under different conditions and exploring the implications of inserting a partition that prevents energy exchange.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the calculation of entropy using the provided multiplicity equations, expressing concerns about the large values resulting from these calculations. Questions arise regarding the relevance of time scales in the context of entropy and the implications of inserting a partition between the solids.

Discussion Status

Some participants are exploring mathematical approaches to simplify the calculations of entropy, while others express confusion about the results and the significance of the findings. There is an ongoing inquiry into the validity of assumptions and the interpretation of the results.

Contextual Notes

Participants note the challenge of dealing with extremely large values in calculations and question whether the problem is intended to yield tractable values for entropy. The relevance of time scales in thermodynamic contexts is also under examination.

Bosley
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Homework Statement


Consider a system of 2 large, identical Einstein solids. Each solid has N=10^23 oscillators, and the total energy units in the combined system is 2N.

a) Assuming that all of the microstates are allowed, compute the entropy of this system. This is the entropy over long time scales.
b) Compute entropy again assuming the system is in its most likely macrostate. This is the entropy over short time scales.
c) Is the issue of time scales really relevant here?
d) Suppose that at a moment when the system is near its most likely macrostate, you insert a partition between the solids so they can't exchange energy anymore. Now, even over long time scales, the entropy is the answer from part a. So the second law of thermodynamics has, in a sense, been violated. Is this significant? Should we lose sleep over it?

Homework Equations


We are given that the multiplicity of the combined system (that is, all possible microstates) is \frac{2^{4N}}{\sqrt{8 \pi N}}.

We're given that the multiplicity of the most likely macrostate (where Energy A = Energy B = N units) is \frac{2^{4N}}{4 \pi N}.

The Attempt at a Solution


a) S = k*log(W)
S = k*log(2^{4*10^{23}}/\sqrt{8*\pi*10^{23}})
Problem: This is incalculably large. Is there some different way that I should be approximating a value for this? Mathematica overflows. Wolfram gives back a nonsensical "power of 10 representation" that is incorrect. What to do?

b) Likewise, S = k*log(2^{4*10^{23}}/(4*\pi*10^{23}) is incalculably large. Does the problem just want me to say "Both are basically infinite"? This is confusing, though, because I thought we were supposed to usually get tractable values for entropy.

c) Since both numbers for a and b are apparently intractably large (unless I'm doing something terribly wrong), it seems that the time scale doesn't matter?

d) I don't know.

Advice please?
 
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Where did you get your multiplicity of the combined system equation?
 
Nevermind. I feel dumb now.
 
Try using log rules. So, for example,

S = k*ln(2^{4*10^{23}}/\sqrt{8*\pi*10^{23}}) becomes
S=k*[(4*10^{23})*ln(2)-(1/2)ln(8*\pi*10^{23})]

And
S = k*log(2^{4*10^{23}}/(4*\pi*10^{23})
Becomes
k*[(4*10^{23})*ln(2)-ln(4*\pi*10^{23})]

Can you evaluate this now?
 

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