What Is the Change in Entropy?

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Discussion Overview

The discussion revolves around a thermodynamics problem involving a system of 100,000 molecules with two energy levels, A and B, and explores concepts such as energy change, heat transfer, and entropy change after a reversible process. Participants analyze the implications of the Boltzmann distribution and the definitions of entropy in the context of the problem.

Discussion Character

  • Homework-related
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant computed the Boltzmann factor and found the energy difference between the two levels to be 2.5*10^-21 J, while another participant suggested a different value of 1.5*10^-21 J, indicating a potential disagreement on significant figures or calculations.
  • There is a discussion about whether multiplying the energy change for one molecule by the number of molecules accurately represents the total energy change, with one participant affirming that it is correct.
  • Concerns are raised regarding the use of the equation ΔS = q/T in the absence of an isothermal condition, with participants noting that the problem specifies a reversible process, which allows for this equation to hold true.
  • Questions arise about the constancy of ΔUab and whether temperature must change during the process, with some participants suggesting that it is implied that ΔUab remains constant while the distribution of molecules changes.
  • There is uncertainty about the integration of dq in relation to temperature changes and how it relates to the calculation of entropy change, with one participant questioning the assumption that temperature can be treated as constant during the integration.
  • Another participant speculates about the possibility of a phase-space path that allows for temperature and entropy changes to occur independently, though this remains unclear.

Areas of Agreement / Disagreement

Participants express differing views on the energy difference calculation and the implications of temperature changes in the context of entropy calculations. The discussion remains unresolved regarding the specifics of the integration and the assumptions made about the process.

Contextual Notes

Limitations include the lack of clarity on the assumptions regarding temperature constancy during the integration of dq and the specific path taken through phase space during the reversible process.

tahaha
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Homework Statement



A system with 100,000 molecules has 2 energy levels, A and B. At first, the 2 energy levels are populated equally. After a reversible process, energy level A is populated by 65% of the molecules and the system is at 293K.

a) What is the difference in energy between the two levels?
b) How much heat was added or removed from the system?
c) What is the change in entropy?

Homework Equations



Boltzmann distribution
Probabilistic definition of entropy

The Attempt at a Solution



I computed the Boltzmann factor for the two energy levels and got the correct answer for (a) = 2.5*10^-21 J.

Then, when I looked at (b) and (c), I thought they wouldn't ask for the change in entropy after asking for the heat, if the change in entropy was required for the calculations of the heat. So I pondered, and got this:

Since in the process, 50%-(100%-65%)=15% of the molecules were transferred from B to A, so the energy change of the process would be= 0.15(100,000)(-ΔUab) = 0.15(100,000)(-2.5*10^-21 J) = -3.75*10^-17 J.

But then I was stuck, because I only had the energy change, and just couldn't find the heat without knowing whether there was work and how much.
And then the solution did what exactly I thought they wouldn't do:

1. Find ΔS using the probabilistic definition:
Initial S= -(100,000)(kb)[2(0.5ln0.5)]
Final S= -(100,000)(kb)[0.65ln0.65 + 0.35ln0.35)]
ΔS= -4570kb

2. ΔS= q/T (reversible)
∴ q= TΔS = -1.85*10^-17 J

Then for (c), they put "see above."

--------

My questions/confusions are:

1). Does my attempt (multiplying the energy change for one molecule by the number of molecules) really get me to the energy change?
2). I'm confused about how they use ΔS= q/T to get the heat here. The problem doesn't say the process is isothermal?

According to the Boltzmann factor:
Nb/Na = exp(-ΔUab/kbT)

The process changes Nb/Na, and ΔUab has to be constant (does it?), T has to change.

-------

I hope the question isn't too long! Thanks for any help!
 
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yeah, it's a tricky problem, more like statistical physics than thermodynamics really.

tahaha said:
I computed the Boltzmann factor for the two energy levels and got the correct answer for (a) = 2.5*10^-21 J.
hmm. I get an energy difference of 1.5*10^-21 J ... Maybe our answers are different because we used different significant figures for our value of the Boltzmann constant. Anyway, you got it correct, so it doesn't matter.

tahaha said:
Does my attempt (multiplying the energy change for one molecule by the number of molecules) really get me to the energy change?
Yep, that is the correct total energy change for the system.

tahaha said:
I'm confused about how they use ΔS= q/T to get the heat here. The problem doesn't say the process is isothermal?
the problem does not say the process is isothermal. The problem only says that the process is reversible, which ensures that the equation ΔS= q/T is true.

tahaha said:
According to the Boltzmann factor:
Nb/Na = exp(-ΔUab/kbT)

The process changes Nb/Na, and ΔUab has to be constant (does it?), T has to change.
yeah. It is meant to be implied that ΔUab is constant. And generally in these kinds of problems, the different possible energy levels are fixed. It is just the number of molecules in each energy level changes.
 
Thanks for clarifying some of my confusions!
But for ΔS= q/T, I thought it was defined as dS=dq(rev.)/T, so you would have to integrate the function to get the entropy change.
If T is not constant, why can you take it out of the integral and simply integrate dq to get q?
Thanks again!
 
yeah, that is strange. I'm not sure about that. Maybe they assume there is a path through phase-space where first, the temperature changes while entropy is constant, then the entropy changes while temperature is constant. And since the heat input is path-independent for a reversible process, if we take any other path through phase space, we still get the same heat input. They don't really say how the system gets from the first part to the second part (apart from saying the process is reversible), so it is hard to say exactly what they had in mind. I guess it is also possible that the difference in the two energy levels does change... It is just quite rare in most problems.
 

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