Statistical Mechanics

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Spring 2020 Vahala
Kate E
Flashcards by Kate E, updated more than 1 year ago
Kate E
Created by Kate E almost 5 years ago
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Question Answer
What is Ω for k indistinguishable elements from n objects with replacement? Ω=nk
What is Ω for k distinguishable elements from n objects without replacement? Ω=n!(nk)!
What is Ω for k indistinguishable elements from n objects without replacement? Ω=(nk)=n!k!(nk)!
Sterling Approximation ln(N!)=Nln(N)N+O(ln(N))
The Microcanonical Interconnect between Statistical Mechanics and Thermodynamics Entropy: S=kbln(Ω)
The Canonical Partition Function for Classical Systems ZCM=1hNNi=1dpidqieH(p,q)β
Microcanonical Partition Function Z=jωjeβEj
Canonical Partition Function Zcan(N,V,T)=1N!1h3N3Ni=1dpidqieH(p,q)β
The Canonical Interconnect between Statistical Mechanics and Thermodynamics Helmholtz Free Energy: F(N,V,T)=kTln(Zcan(N,V,T))
The Grand Canonical Partition Function ZG=eλZcan
where λ=eμ/kT is the "fugacity"
The Grand Canonical Interconnect between Statistical Mechanics and Thermodynamics The Grand Potential: Φ(T,V,μ)=pV=kTln(ZG)
Characteristic of Microcanonical Ensembles Every state is equally probable.
Characteristic of Canonical Ensembles Energy is allowed to fluctuate.
Characteristic of Grand Canonical Ensembles Energy and particle number are allowed to fluctuate.
The Canonical Equation for Entropy S=T(Tln(Zcan))
The Canonical Equation for Internal Energy U=kbT2Tln(Zcan)
The Grand Canonical Equation for Total Particle Number N=kbTμln(ZG)
The Grand Canonical Equation for Fluctuations in Particle Number (ΔN)2=2(μβ)2ln(ZG)
/[dE/] /[dE=T\;dS-P\;dV+\mu\;dN/]
dF
dF=SdTPdV+μdN
F=ETS
CV
TST|V,N=ET|V,N
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