Rushbrooke inequality

From Wikipedia, the free encyclopedia
Jump to: navigation, search

In statistical mechanics, the Rushbrooke inequality relates the critical exponents of a magnetic system which exhibits a first-order phase transition in the thermodynamic limit for non-zero temperature T.

Since the Helmholtz free energy is extensive, the normalization to free energy per site is given as

The magnetization M per site in the thermodynamic limit, depending on the external magnetic field H and temperature T is given by

where is the spin at the i-th site, and the magnetic susceptibility and specific heat at constant temperature and field are given by, respectively



The critical exponents and are defined in terms of the behaviour of the order parameters and response functions near the critical point as follows


measures the temperature relative to the critical point.


For the magnetic analogue of the Maxwell relations for the response functions, the relation

follows, and with thermodynamic stability requiring that , one has

which, under the conditions and the definition of the critical exponents gives

which gives the Rushbrooke inequality

Remarkably, in experiment and in exactly solved models, the inequality actually holds as an equality.