In the finite-deformation, continuum theory of crystal plasticity, the latt
ice is assumed to distort only elastically, while generally the elastic def
ormation itself is not compatible with a single-valued displacement field.
Lattice incompatibility is shown to be characterized by a certain skew-symm
etry property of the gradient of the elastic deformation field, and this me
asure can play a natural role in a nonlocal, gradient-type theory of crysta
l plasticity. A simple constitutive proposal is discussed where incompatibi
lity only enters the instantaneous hardening relations, and thus the increm
ental moduli, which preserves the classical structure of the incremental bo
undary value problem. (C) 2000 Elsevier Science Ltd. All rights reserved.