Canonical ensemble

Canonical Ensemble:

Variables:

• Number of Particles, $N$

• Volume, $V$

• Temperature, $T$

Partition Function

Classical Partition Function (one-component system) in a three-dimensional space: $Q_{NVT}$

$Q_{NVT}=\frac{V^N}{N!{\mathrm{\Lambda }}^{3N}}\int d(R^{*}{)}^{3N}\exp [-\beta U(V,(R^{*}{)}^{3N})]$

where:

• $\mathrm{\Lambda }$ is the de Broglie wavelength

• $\beta =\frac{1}{k_{B}T}$, with $k_B$ being the Boltzmann constant,

• $U$ is the potential energy, which depends on the coordinates of the particles (and on the interaction model)

• ${(R^{*})}^{3N}$ represent the 3N position coordinates of the particles (reduced with the system size): i.e. $\int d(R^{*}{)}^{3N}=1$

Free energy and Partition Function

The Helmholtz free energy is related to the canonical partition function as:

$F(N,V,T)=-\log Q_{NVT}$