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!(n−k)! |
What is Ω for k indistinguishable elements from n objects without replacement? |
Ω=(nk)=n!k!(n−k)! |
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=1hN∫⋯∫N∏i=1dpidqie−H(p,q)β |
Microcanonical Partition Function |
Z=∑jωjeβEj |
Canonical Partition Function |
Zcan(N,V,T)=1N!1h3N∫3N∏i=1dpidqie−H(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=kbT2∂∂Tln(Zcan) |
The Grand Canonical Equation for Total Particle Number |
N=kbT∂∂μln(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=−SdT−PdV+μdN
F=E−TS |
CV |
T∂S∂T|V,N=∂E∂T|V,N |
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