Experimental and theoretical research of the last few years have shown that
it is impossible in principle to describe macroscopic properties of plasti
c flow when only the dislocation theory is adopted. It is necessary to take
into consideration one or more intermediate mesoscopic levels at which vol
umes of finite sizes are the objects of study. The heterogeneity of a mater
ial's internal structure and formation of substructures of essentially a gr
eater scale than separate dislocation are to be taken into account obviousl
y during plastic deformation in mesovolumes, Hence, an adequate model of th
e mesovolume behaviour should consider displacement, rotations and interact
ion of structural elements. which are available in the mesovolume, A medium
like this requires to take account of internal non-compensated moments and
only for a representative mesovolume the total (averaged) moment is equal
to zero, A simple model is offered here which allows one to consider indepe
ndent rotations of mesofragments of finite size without obvious calculation
of couple-stress and torsion-curvature. As rotation and displacement of in
dividual mesofragment, and its strain as well, are completely determined by
its velocity field, it is necessary to define an asymmetrical part of the
force-stress tenser from additional physical reasons, It is supposed in the
model that at the stage of perfectly elastic deformation the stress tenser
is symmetric, and its asymmetrical part appears only at the stage of plast
ic deformation and is proportional to the function of plastic strain accumu
lated in the considered local area. Test calculations carried out have show
n that the model is able to simulate the behaviour of crystals with a limit
ed number of active slip systems well. In the case of two-dimensional flow.
a spin parameter determines both magnitude and direction (by the sign of t
he parameter) of rotation of local mesovolumes of a material. (C) 2000 Else
vier Science B.V, All rights reserved.