It is obvious that the exact solutions of the evolution equation, which is derived by
regarding the deformation process of viscoelastic materials as an irreversible themodynamic process,
depend very much on the properties of their coefficient matrices. These matrices are usually affected
by the nature of the generalized thermodynamic coordinates, say, the number and location of the
neutrally stable equilibrium coordinates and those participating in the entropy production of the
isolated system. These provide us a ground to distinguish the ideal viscoelastic solid state and the
ideal viscoelastic fluid state in creep or stress relaxation behaviour.