The structure of Maxwell relations is a statement of equality among the second derivatives for continuous functions. It follows directly from the fact that the order of differentiation of an analytic function of two variables is irrelevant (Schwarz theorem). In the case of Maxwell relations the function considered is a thermodynamic potential and xi and xj are two different natural variables for that potential:
Schwarz' theorem (general)
where the partial derivatives are taken with all other natural variables held constant. It is seen that for every thermodynamic potential there are n(n − 1)/2 possible Maxwell relations where n is the number of natural variables for that potential.
The substantial increase in the entropy will be verified according to the relations satisfied by the laws of thermodynamics
The four most common Maxwell relations are the equalities of the second derivatives of each of the four thermodynamic potentials, with respect to their thermal natural variable (temperatureT; or entropyS) and their mechanical natural variable (pressureP; or volumeV):
where the potentials as functions of their natural thermal and mechanical variables are the internal energyU(S, V), enthalpyH(S, P), Helmholtz free energyF(T, V) and Gibbs free energyG(T, P). The thermodynamic square can be used as a mnemonic to recall and derive these relations. The usefulness of these relations lies in their quantifying entropy changes, which are not directly measurable, in terms of measurable quantities like temperature, volume, and pressure.
Consider, the equation . We can now immediately see that
Since we also know that for functions with continuous second derivatives, the mixed partial derivatives are identical (Symmetry of second derivatives), that is, that
we therefore can see that
and therefore that
Derivation of Maxwell Relation from Helmholtz Free energy
The differential form of Helmholtz free energy is
From symmetry of second derivatives
and therefore that
The other two Maxwell relations can be derived from differential form of enthalpy and the differential form of Gibbs free energy in a similar way. So all Maxwell Relationships above follow from one of the Gibbs equations.
Combined form first and second law of thermodynamics,
U, S, and V are state functions.
Substitute them in Eq.1 and one gets,
And also written as,
comparing the coefficient of dx and dy, one gets
Differentiating above equations by y, x respectively
U, S, and V are exact differentials, therefore,
Subtract eqn(2) and (3) and one gets
Note: The above is called the general expression for Maxwell's thermodynamical relation.
as a statement about differential forms, and take the exterior derivative of this equation, we get
since . This leads to the fundamental identity
The physical meaning of this identity can be seen by noting that the two sides are the equivalent ways of writing the work done in an infinitesimal Carnot cycle. An equivalent way of writing the identity is
The Maxwell relations now follow directly. For example,
The critical step is the penultimate one. The other Maxwell relations follow in similar fashion. For example,
The above are not the only Maxwell relationships. When other work terms involving other natural variables besides the volume work are considered or when the number of particles is included as a natural variable, other Maxwell relations become apparent. For example, if we have a single-component gas, then the number of particles N is also a natural variable of the above four thermodynamic potentials. The Maxwell relationship for the enthalpy with respect to pressure and particle number would then be:
where μ is the chemical potential. In addition, there are other thermodynamic potentials besides the four that are commonly used, and each of these potentials will yield a set of Maxwell relations.
Each equation can be re-expressed using the relationship
which are sometimes also known as Maxwell relations.