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

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SUMMARY

The discussion centers on the internal energy function U(S,V,A,N) expressed as U=TS-PV+γA+μN. The total differential is derived as dU=TdS-PdV+γdA+μdN for a one-component system, with the condition that dT=dP=dγ=dμ=0, indicating these variables are intensive properties. The conversation also references the Gibbs formulation and Legendre transforms, highlighting their relevance in thermodynamics. Key literature includes "Basic Thermodynamics" by Carrington and various Physical Chemistry texts.

PREREQUISITES
  • Understanding of thermodynamic concepts such as internal energy and total differentials.
  • Familiarity with intensive and extensive properties in thermodynamics.
  • Knowledge of Legendre transforms and their application in thermodynamic equations.
  • Basic principles of the Gibbs formulation in thermodynamics.
NEXT STEPS
  • Study the derivation of thermodynamic potentials using Legendre transforms.
  • Explore the Gibbs formulation in detail, focusing on its applications in physical chemistry.
  • Review the concept of intensive vs. extensive properties in thermodynamics.
  • Examine the relationship between partial derivatives and thermodynamic variables in various contexts.
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Students and professionals in thermodynamics, physical chemistry, and related fields, particularly those looking to deepen their understanding of internal energy and its mathematical representations.

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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