The Cauchy stress tensor, T-ij, is considered for an elastic material which
is subject to any internal isotropic constraint, apart from the constraint
of incompressibility. For a given strain, it is seen that if in a given ba
sis one of the eigenvectors of the stress tensor has a zero component, say
the alpha th component, and if the arbitrary scalar term in the stress may
be chosen so that T-alpha beta(alpha not equal beta) shear stress component
is zero, then the stress tensor has a double eigenvalue. This means that t
here is a great simplification in the stress field. The given strain may be
maintained experimentally by a simple tension superimposed upon a hydrosta
tic stress field. Examples are presented for Bell-constrained and Ericksen-
constrained materials.