Partial Derivatives of U w.r.t. T and ##\mu## at Fixed N

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Homework Help Overview

The discussion revolves around the partial derivatives of internal energy \( U \) with respect to temperature \( T \) and chemical potential \( \mu \) while keeping the number of particles \( N \) fixed. The original poster seeks to understand the relationship expressed in a formula from a textbook, which involves derivatives of \( U \) with respect to multiple variables.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the implications of taking partial derivatives while holding different variables constant. There are questions about the validity of the formula and how to derive the terms correctly. Some participants suggest that the book's approach may lead to ambiguity in defining changes in \( U \) due to the multi-dimensional nature of the variables involved.

Discussion Status

The discussion is ongoing, with participants sharing insights and seeking clarification on the mathematical framework. Some have received guidance from a professor regarding the conditions under which certain variables should be held constant, which appears to have aided understanding for at least one participant.

Contextual Notes

There are mentions of the need to hold specific variables constant when taking derivatives, particularly in relation to the context of thermodynamic potentials. The complexity of the relationships among \( N \), \( \mu \), and \( T \) is acknowledged, leading to discussions about the mathematical soundness of the original formula presented in the homework statement.

Silviu
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Homework Statement


Show that ##\frac{\partial U}{\partial T}|_{N} = \frac{\partial U}{\partial T}|_{\mu} + \frac{\partial U}{\partial \mu}|_{T} \frac{\partial \mu}{\partial T}|_{N} ## (Pathria, 3rd Edition, pg. 197)

Homework Equations


##U=TS + \mu N - pV##

The Attempt at a Solution


I tried to take the derivative of U with respect with T at constant N and then at constant ##\mu## but I can't get the term on the right. I am not sure how can I get a product of 2 derivatives, because in taking derivatives in ##U=TS + \mu N - pV## I always have a derivative times a number (for example ##T\frac{\partial S}{\partial T}|_N##). What should I do? Is there another way other than using this formula?
 
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Just a suggestion=perhaps the book is correct, but they appear to be using ## U=U(N,\mu,T) ##, so that in taking ## \frac{\partial{}}{\partial{T}} ##, both ## N ## and ## \mu ## should be held constant.
 
Charles Link said:
Just a suggestion=perhaps the book is correct, but they appear to be using ## U=U(N,\mu,T) ##, so that in taking ## \frac{\partial{}}{\partial{T}} ##, both ## N ## and ## \mu ## should be held constant. Likewise for the other partial derivatives.
OK, But does this leads to having a term with 2 derivatives. I might have stuff like ##\frac{\partial U}{\partial T}|_{N,\mu}## or something similar, but I still don't see how do I get a product of 2 derivatives. Thank you!
 
Silviu said:
OK, But does this leads to having a term with 2 derivatives. I might have stuff like ##\frac{\partial U}{\partial T}|_{N,\mu}## or something similar, but I still don't see how do I get a product of 2 derivatives. Thank you!
I'm going to need to study it further. It looks like it might take a little work if it is correct.
 
Charles Link said:
I'm going to need to study it further. It looks like it might take a little work if it is correct.
With a little further thought, it seems taking a partial with only holding one other variable constant is ambiguous, because on the multi-dimensional surface, you can not precisely define how much the quantity ## U ## will change. It allows multiple paths depending on what you do with the 3rd variable. @Chestermiller Might you offer an input here?
 
Charles Link said:
With a little further thought, it seems taking a partial with only holding one other variable constant is ambiguous, because on the multi-dimensional surface, you can not precisely define how much the quantity ## U ## will change. It allows multiple paths depending on what you do with the 3rd variable. @Chestermiller Might you offer an input here?
But even if you keep 2 constant at each derivation, I am still not sure how to prove it.
 
Silviu said:
But even if you keep 2 constant at each derivation, I am still not sure how to prove it.
If you look at the term on the left and the first term on the right, if you include the third variable in both of the partial derivatives to be held constant, these two are then the same. IMO the equation is mathematically unsound, but perhaps @Chestermiller can add to that and/or possibly concur.
 
U is typically a function of 3 parameters, usually S, V, and N. So two parameters need to be held constant in those partial derivatives. What is the other parameter?
 
Chestermiller said:
U is typically a function of 3 parameters, usually S, V, and N. So two parameters need to be held constant in those partial derivatives. What is the other parameter?
The author is using ## N ## , ## \mu ##, and ## T ## as the 3 parameters, but he's only holding one constant at a time. To me this appears to be mathematically unsound.
 
  • #10
Charles Link said:
The author is using ## N ## , ## \mu ##, and ## T ## as the 3 parameters, but he's only holding one constant at a time. To me this appears to be mathematically unsound.
I asked my professor and he told me that for ##C_n## N and V must be held constant and for ##C_\mu##, ##\mu## and V must be held constant in order to solve the problem. Does this help?
 
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  • #11
Silviu said:
I asked my professor and he told me that for ##C_n## N and V must be held constant and for ##C_\mu##, ##\mu## and V must be held constant in order to solve the problem. Does this help?
That is very helpful=I solved it now=I will post it momentarily. ## \\ ##
## U=U(N,T,V) ## and ## N=N(\mu,T,V) ## so that ## U=U(\mu,T,V) ## and ## \mu=\mu(N,T,V) ##. ## \\ ##
## (\frac{\partial{U(N,T,V)}}{\partial{T}})_{N,V}=(\frac{\partial{U(\mu,T,V)}}{\partial{T}})_{N,V}=(\frac{\partial{U(\mu,T,V)}}{\partial{\mu}})_{T,V}(\frac{\partial{\mu(N,T,V)}}{\partial{T}})_{N,V}+(\frac{\partial{U(\mu,T,V)}}{\partial{T}})_{\mu,V} ##. ## \\ ##
Yes, your professor's input was very helpful. (Note: Ten minutes after posting= I just edited the T, V subscript in the first term after the second "=" sign from an incorrect N,V subscript)
 
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  • #12
@Silviu Please see the latest editing on the previous post.
 
  • #13
Charles Link said:
@Silviu Please see the latest editing on the previous post.
Thank you so much for help. But I am a bit confused about the math behind it. Is this like a chain rule, when you keep some variable constants?
 
  • #14
Silviu said:
Thank you so much for help. But I am a bit confused about the math behind it. Is this like a chain rule, when you keep some variable constants?
Very much so=the chain rule. You go through the list of variables and take the appropriate derivatives, and skip over any variables that are held constant.
 
  • #15
Charles Link said:
Very much so=the chain rule. You go through the list of variables and take the appropriate derivatives, and skip over any variables that are held constant.
OK, makes sense. Thank you so so much!
 
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