We develop a micromechanical theory of dislocation structures and finite de
formation single crystal plasticity based on the direct generation of defor
mation microstructures and the computation of the attendant effective behav
ior. Specifically, we aim at describing the lamellar dislocation structures
which develop at large strains under monotonic loading. These microstructu
res are regarded as instances of sequential lamination and treated accordin
gly. The present approach is based on the explicit construction of microstr
uctures by recursive lamination and their subsequent equilibration in order
to relax the incremental constitutive description of the material. The mic
rostructures are permitted to evolve in complexity and fineness with increa
sing macroscopic deformation. The dislocation structures are deduced from t
he plastic deformation gradient field by recourse to Kroner's formula for t
he dislocation density tensor. The theory is rendered nonlocal by the consi
deration of the self-energy of the dislocations. Selected examples demonstr
ate the ability of the theory to generate complex microstructures, determin
e the softening effect which those microstructures have on the effective be
havior of the crystal, and account for the dependence of the effective beha
vior on the size of the crystalline sample, or size effect.. In this last r
egard, the theory predicts the effective behavior of the crystal to stiffen
with decreasing sample size, in keeping with experiment. Tn contrast to st
rain-gradient theories of plasticity, the size effect occurs for nominally
uniform macroscopic deformations. Also in contrast to strain-gradient theor
ies, the dimensions of the microstructure depend sensitively on the loading
geometry, the extent of macroscopic deformation and the size of the sample
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