“…Essentially, a neutral change of state of a perfect crystal corresponds to a lattice matrix L(u(x)) = Vu(x){Vv(x)}-i, where u : Q. -»[R 3 is the elastic deformation, Cl is the reference configuration and v represents the slip or plastic deformation with det Vv = 1 a. e. in £1 ERICKSEN [13] and DAVINI & PARRY [10] have discussed the likelyhood that crystal equilibria correspond to some kind of variational principle, and offered the opinion that the relevant class of variations should encompass, at the most, the elastic changes and the rearrangements, so excluding any change of state which alters the invariants. In this paper we study the implications of including neutral changes of state in the class of admissible variations while taking the viewpoint that equilibria correspond to minimizers of an energy functional E(u, v) := Jw(Vu(x){ Vv(x)}' 1 ) dx (1.2)…”