Entropy & Free Energy Change: Understanding at Equilibrium

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Discussion Overview

The discussion revolves around the concepts of entropy and free energy change at equilibrium, exploring the definitions and implications of "change" in these contexts. Participants examine the relationship between equilibrium states and the rates of change of these thermodynamic quantities, with references to thermodynamic principles and calculus.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question how "change" in entropy can be defined at an instant, suggesting that a comparison to another state is necessary.
  • Others propose that the "rate of change of entropy" at equilibrium is what is meant, indicating that the first derivative of entropy with respect to time is zero.
  • One participant introduces the idea that the relationship between entropy and information is complex, using examples of gas distribution in different gravitational fields.
  • Several participants discuss the fundamental thermodynamic relation and its implications for calculating changes in entropy and free energy.
  • There is a suggestion that the term "change" may often refer to "rate of change," particularly in the context of free energy, where the first derivative with respect to time is also zero at equilibrium.
  • Some participants express that the original text may not clearly indicate the relationship between change and time, leading to confusion.
  • A later reply clarifies that if the time rate of change is zero, it implies that future change in entropy may also be zero, although this is debated.
  • One participant suggests that the statement regarding free energy change at equilibrium could be more accurately described as a difference in free energies of reactants and products being zero.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of "change" in the context of entropy and free energy. While some agree on the importance of considering rates of change, others highlight ambiguities in the original text and the implications of time in these definitions. The discussion remains unresolved regarding the clarity of these concepts.

Contextual Notes

Limitations include potential ambiguities in the definitions of change and the relationship to time, as well as varying interpretations of thermodynamic principles across different texts.

springwave
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"change" in entropy

While reading a textbook on introductory thermodynamics , I came across the following-

"When a system is in equilibrium, the entropy is maximum and the change in entropy ΔS is zero "
And also

"We can say that for a spontaneous process, entropy increases till it reaches a maximum, at equilibrium where the change in entropy is zero "

(here entropy refers to total entropy, ie system plus surroundings)

I fail to understand how one can define "change" for an instant.
Like "change of entropy is zero at equilibrium". To define change we need to compare two different states. In this case, equilibrium is one of the states. What is the other state to which it is being compared to? Is it the initial state of the system?

How do we calculate this "change in entropy", at various instants of the process? Can we write it as a function of time?

(I have the same problem with free energy, they always say "change in free energy is zero at equilibrium")
 
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It's not just 'change for an instant'...try reading the first two sections here:

http://en.wikipedia.org/wiki/Second_law_of_thermodynamics

and see if that clarifies it for you. See the first formula.

but be prepared, 'entropy' is very tricky!

Here is one idea I did not uncover for quite a while:

The relationship between entropy and information is subtle and complex.

Suppose I give you a box of gas and ask you what you think the distribution of the gas is. A logical guess is equally dispersed, right? That would not be a surprising answer...the gas diffuses and reaches an equilibrium [maximum entropy] unless disturbed.

Now let's put it in a really strong gravitational field and give the field time to reach equilibrium: now the "most likely" state would be "clumpy", maybe like the universe...again entropy is maximum...[I don't think anybody really understands entropy yet...like gravity, maybe...That's why John von Neumann suggested to Claude Shannon when Shannon was developing information theory at Bell Labs he use entropy instead of "uncertainty" in explanations...opponents would be intimidated because nobody knows what 'entropy' is! ]
 
Last edited:


springwave said:
While reading a textbook on introductory thermodynamics , I came across the following-

"When a system is in equilibrium, the entropy is maximum and the change in entropy ΔS is zero "
And also

"We can say that for a spontaneous process, entropy increases till it reaches a maximum, at equilibrium where the change in entropy is zero "

(here entropy refers to total entropy, ie system plus surroundings)

I fail to understand how one can define "change" for an instant.
Like "change of entropy is zero at equilibrium". To define change we need to compare two different states. In this case, equilibrium is one of the states. What is the other state to which it is being compared to? Is it the initial state of the system?

How do we calculate this "change in entropy", at various instants of the process? Can we write it as a function of time?

(I have the same problem with free energy, they always say "change in free energy is zero at equilibrium")
They meant the "rate of change of entropy", not the "change in entropy". At thermal equilibrium, the first derivative of entropy with respect to time is zero.

In other words,
0=dS/dt,
where S is the entropy of the system at equilbrium and t is the time.

This would be a "total" derivative and not a partial derivative. The physical quantity called entropy is not changing. That is why I chose "d" instead of "∂" in the expression.

Sometimes, writers use the word "change" when they really mean "rate of change".
 


springwave said:
I fail to understand how one can define "change" for an instant.
Change for an instant? What do you think calculus is based on? :-p

As for calculation, fundamental thermodynamic relation can be given by dU = TdS - PdV, where dU, dS, and dV are infinitesimal changes in potential energy, entropy, and volume (respectively).
 


Mandelbroth said:
Change for an instant? What do you think calculus is based on? :-p
I was going to say that!

As for calculation, fundamental thermodynamic relation can be given by dU = TdS - PdV, where dU, dS, and dV are infinitesimal changes in potential energy, entropy, and volume (respectively).
 


springwave said:
(I have the same problem with free energy, they always say "change in free energy is zero at equilibrium")
Again, the book's mean "rate of change of free energy is zero at equilibrium." Or rather, "the first derivative of the free energy with respect to time is zero at equilibrium."
dG/dt=0
where G is the free energy and t is the time. The letter "d" stands for "differential."

The "derivative" is a concept from calculus. It can be expressed as:
lim [dt→0] ={G(t+dt)-G(t)}/dt.
where lim[] is the limit operator wiht respect to whatever is in the [], t is a specific time, dt is an increment of time.

One sees that there is a "comparison" implied by the derivative operator. By saying the "rate of change of free energy is zero," one is also saying that there is a always and δ>0 for every ε> such that if dt<δ:
|G(t+dt)-G(t)|< ε|dt|.
Any time you evaluate a limit, you are making a comparison between two quantities. So the derivative of free energy with respect to time also implies a comparison between two values of free energy at slightly different times.

"Equilibrium" means the state of not changing in time with time. Calculus just formalizes the concept.
 


If the time rate of change is zero then surely future change ΔS is also zero?

There was nothing in the OP quotes from his book that was time related. The introduction of 'instant' was his own.
 


Studiot said:
If the time rate of change is zero then surely future change ΔS is also zero?

There was nothing in the OP quotes from his book that was time related. The introduction of 'instant' was his own.
That may well be a problem with the book rather than the OP. Some writers forget to say with what independent variable the "change" in the dependent variable is associated with.

Nevertheless, there are many textbooks and other references that state explicitly that the "change" is with respect to time. An equilibrium state is one that doesn't change with time.
 


Thanks for the help guys! I guess I understand it better now.

What he probably meant in the book by ΔG was the difference in absolute free energies of reactants and products at equilibrium was zero, and as mentioned on the wikipedia page it can be proved that

ΔG(between reactants and products) = d(G)/dε (where ε is reaction coordinate) (I guess activity)

Hence, similar to what Darwin123 said if d(G)/dt is zero, d(G)/dε is also zero, and hence ΔG is also zero.

So may be the statement "difference" in free energies (of reactants and products) at equilibrium would more descriptive than "change in free energy".

For entropy I guess what the text meant was that dS/dt is zero at equilibrium (like Darwin123 said)
 

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