Deriving heat capacity using thermodynamics identity

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ultimateguy
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Homework Statement


Use the thermodynamic identity to derive the heat capacity formula [tex]C_V=T\frac{\partial{S}}{\partial{T}}_V[/tex]

Homework Equations


[tex]C_V=\frac{\partial{U}}{\partial{T}}[/tex]
[tex]T=\frac{\partial{U}}{\partial{S}}[/tex]
dU=TdS-PdV+[tex]\mu[/tex]dN

The Attempt at a Solution



I used [tex]C_V=\frac{\partial{U}}{\partial{S}}\frac{\partial{S}}{\partial{T}}=T\frac{\partial{S}}{\partial{T}}_V=\frac{\partial{U}}{\partial{T}}=C_V[/tex].
This is the only solution I can think of, but I don't think I used the thermodynamics identity, did I?
 
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There are a distinct lack of thermal physicists on this website and with good reason as it is one of the most boring subjects ever. I think if you know that:

[tex]dS=(\frac{\partial{S}}{\partial{U}})_{PV}dU[/tex]

Then you can substitute the following into the equation for dU,

[tex]dU=(\frac{\partial{U}}{\partial{T}})_VdT[/tex]

and have a fiddle about, that should set you off on the right lines.
 
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This may be a dumb question, but what's the difference between E and U?
 
ultimateguy said:
This may be a dumb question, but what's the difference between E and U?

There is none. I apologise. I normally write E and I was trying to conform to your notation but obviously forgot half way through I will change it.
 
I'd have thought if they wanted a derivation from the thermodynamic identity then they'd want you to start from that. However the OP proof might be accepted.