Microcanonical ensemble

The statistical ensemble of isolated systems with fixed energy, particle number, and volume.
Microcanonical ensemble

The microcanonical ensemble describes an isolated thermodynamic system with fixed total energy EE, particle number NN, and volume VV.

Classical formulation

The ensemble assigns equal probability to all in a thin energy shell:

ρ(q,p)=1Ω(E,V,N)δ(H(q,p)E) \rho(q, p) = \frac{1}{\Omega(E, V, N)} \delta(H(q,p) - E)

where Ω\Omega is the and HH is the .

Microcanonical entropy

The is

S(E,V,N)=kBlnΩ(E,V,N) S(E, V, N) = k_B \ln \Omega(E, V, N)

where Ω\Omega counts the number of accessible microstates (or phase space volume).

Thermodynamic quantities

Temperature and pressure emerge from entropy derivatives:

1T=SEV,N,PT=SVE,N. \frac{1}{T} = \frac{\partial S}{\partial E}\bigg|_{V,N}, \quad \frac{P}{T} = \frac{\partial S}{\partial V}\bigg|_{E,N}.

Relation to other ensembles

In the , the microcanonical ensemble is equivalent to the and ensembles for typical observables.