Internal Energy as a function of U(S,V,A,Ni)

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The discussion centers on the relationship between internal energy (U) and its variables, specifically how the total differential dU is expressed as dU = TdS - PdV + γdA + μdN for a one-component system. The key question raised is why the differentials of temperature (dT), pressure (dP), surface tension (dγ), and chemical potential (dμ) are considered to be zero in this context, suggesting they are intensive properties or potentials. The conversation also touches on the derivation of temperature as the partial derivative of internal energy with respect to entropy (T = ∂U/∂S) and the relevance of Legendre transforms in this framework. Additionally, references to authoritative texts on thermodynamics and physical chemistry are made to support the discussion.
mcoth420
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A general thermo question...
for the function describing internal energy U(S,V,A,N)

U=TS-PV+γA+μN

please explain how the total differential is

dU=TdS-PdV+γdA+μdN (for a one component system)

Basically why is dT=dP=dγ=dμ=0? Is it because they are intensive or potentials?

Thank you,

M
 

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Does this help?


\begin{array}{l}<br /> U = U(S,V,.N,A...) \\ <br /> dU = {\left( {\frac{{\partial U}}{{\partial S}}} \right)_{V,N,A...}}dS + {\left( {\frac{{\partial U}}{{\partial V}}} \right)_{S,N,A}}dV... \\ <br /> T = {\left( {\frac{{\partial U}}{{\partial S}}} \right)_{V,N,A...}} \\ <br /> P = {\left( {\frac{{\partial U}}{{\partial V}}} \right)_{S,N,A}} \\ <br /> {\rm{etc}} \\ <br /> \end{array}

I will leave you to fill in the bits for moles and area or other quantities.
 
Thank you for your reply...what is this technique called? I am working with Legendre transforms and this is similar...

Another thing...how can you derive T=partialU/partialS or others without knowledge of the internal energy equation?
 
This is the Gibbs Formulation.

Carington : Basic Thermodynamics P 187ff : Oxford University Press

Also in many Physical Chemistry texts.
 
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