2.2 Elements of the constitutive theory
Since, however, the constitutive functions and π are generally not explicitly known, the major
task of thermodynamics is the determination of these functions, or at least the restriction of their generality.
In simple cases it is possible to reduce the constitutive functions to a few coefficients which may be turned
over to the experimentalist for measurement. The formulation and exploitation of such restrictions is the
subject of the constitutive theory.
The tools of the constitutive theory are certain universal physical principles which have come
to be accepted by the extrapolation of common experience. Above all there are three such
principles:

The Entropy Inequality.
 The entropy density and the entropy flux combine to form a
fourvector , whose divergence is equal to the entropy production . The
fourvector and are both constitutive quantities and is assumed nonnegative
for all thermodynamic processes. Thus we may write , and
This inequality is clearly an extrapolation of the entropy inequalities known in thermostatics and
thermodynamics of irreversible processes; it was first stated in this generality by Müller
[36, 38].

The Principle of Relativity.
 The principle of relativity requires that the field equations and the entropy
inequality have the same form in all
 Galilei frames for the nonrelativistic case, or in all
 Lorentz frames for the relativistic case.
The formal statement and exploitation of this principle have to await a specific choice for the fields
and the fourfluxes .

The Requirement of Concavity of the Entropy Density.

It is possible, and indeed common, to make a specific choice for the fields and the concavity
postulate is contingent upon that choice.
 In the nonrelativistic case we choose the fields as the densities . The requirement of
concavity demands that the entropy density be a concave function of the variables :
 In the relativistic case we choose the fields as the densities in a generic
Lorentz frame that moves with the fourvelocity with respect to the observer. We have
and . We cannot be certain that in all these frames the entropy density
is concave as a function of . Therefore we assume that there is at least one
– a privileged one, denoted by – such that is concave with respect to
, viz.
The privileged covector remains to be chosen, see Section 4.1.
In both cases the concavity postulate makes it possible that the entropy be maximal for a
particular set of fields – the set corresponding to equilibrium – and that is its attraction for
physicists. For mathematicians the attraction of the concavity postulate lies in the observation
that concavity implies symmetric hyperbolicity of the field equations, see Sections 3.2 and 4.2
below.