Another question from Ashcroft and Mermin: Fermi-Dirac Distribution

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SUMMARY

The discussion centers on the relationship between the Helmholtz free energy (F) and the energy expression E(a,N) as presented in Ashcroft and Mermin's book. Specifically, it highlights that F is defined as F = U - TS, where U is internal energy and TS is the product of temperature and entropy. The canonical ensemble partition function Q(N, V, T) is crucial for calculating F, as it is expressed as F(N, V, T) = -kT lnQ(N, V, T). This relationship is fundamental in statistical thermodynamics.

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  • Knowledge of canonical ensemble partition functions
  • Basic principles of Fermi-Dirac statistics
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Students and researchers in physics, particularly those focusing on statistical mechanics and thermodynamics, as well as anyone seeking to deepen their understanding of Fermi-Dirac statistics and energy relationships in N-electron systems.

hagopbul
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this time about fermi -dirac distribution
Good Day :

i reached the page 40 of Ashcroft Mermin book and after the equation 2.38 there is this expression of E(a,N) which is equal to Helmoltez Free energy F = U - TS , how this two terms F , E are related ? anyone can provide adequate explanation , and few useful references

Best Regards
HB
 
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I do not have the book. What is a ?
 
ath stationary state of N-electron system
 
hagopbul said:
Summary:: this time about fermi -dirac distribution

i reached the page 40 of Ashcroft Mermin book and after the equation 2.38 there is this expression of E(a,N) which is equal to Helmoltez Free energy F = U - TS , how this two terms F , E are related ? anyone can provide adequate explanation , and few useful references
The sum in the denominator of eq. 2.38 is the “canonical ensemble partition function” Q(N, V, T) of the considered N-electron system at volume V and temperature T. From statistical thermodynamics one has for the Helmholtz free energy F(N, V, T) of a closed system: F(N, V, T) = -kT lnQ(N, V, T)

https://en.wikipedia.org/wiki/Helmholtz_free_energy
 
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