Characteristic state function

The characteristic state function in statistical mechanics refers to a particular relationship between the partition function of an ensemble.

In particular, if the partition function P satisfies

$P=\exp(-\beta Q)$ or $P=\exp(+\beta Q)$

in which Q is a thermodynamic quantity, then Q is known as the "characteristic state function" of the ensemble corresponding to "P". Beta refers to the thermodynamic beta.

Examples

• The microcanonical ensemble satisfies $\Omega (U,V,N)=e^{{\beta TS}}\;\,$ hence, its characteristic state function is $TS$.
• The canonical ensemble satisfies $Z(T,V,N)=e^{{-\beta A}}\,\;$ hence, its characteristic state function is the Helmholtz free energy $A$.
• The grand canonical ensemble satisfies ${\mathcal Z}(T,V,\mu )=e^{{-\beta \Phi }}\,\;$, so its characteristic state function is the Grand potential $\Phi$.
• The isothermal-isobaric ensemble satisfies $\Delta (N,T,P)=e^{{-\beta G}}\;\,$ so its characteristic function is the Gibbs free energy $G$.

State functions are those which tell about the equilibrium state of a system