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140
THREE-DIMENSIONAL PROBLEM OF THE
MATHEMATICAL
THEORY OF PLASTICITY
Y.N. Radayev, Department of Continuum Mechanics, Samara State University, Samara
443011, Russia
Three-dimensional static and kinematic equations of the theory of perfect elastoplastic
ity are considered in an attempt to find approaches to analytical study of three-dimensional
elastic-plastic problems. The Tresca yielding criterion and associated flow rule are employed
to formulate the closed system of equations. If an actual stress state corresponds to an edge
of the Tresca prism then the stress tensor are determined by the maximal (or minimal) prin
cipal stress and the unit vector field directed along the principal stress axis associated with
that principal stress, thus allowing the static equilibrium equations to be formally considered
independently of kinematic. As it is shown, these equations are of hyperbolic type that pro
vides significant mathematical advantages for the present theory. An important geometrical
property of that unit vector field can be derived by analyzing the static equilibrium equa
tions: necessarily it is of complex-lamelar type. It is then found that the complex-lamelar
unit vector field, co-oriented to the principal stress axis, determines a special curvilinear co
ordinate system (the Lame isostatic co-ordinate net). The latter is the most appropriate for
further considerations as transformed static equations can be readily integrated providing
a remarkable development of the theory of three-dimensional plasticity. Since the curvilin
ear co-ordinate system generates a canonical transformation of spatial domains then the
canonical transformation technique applicable to three-dimensional, plane strain and axi
ally-symmetric problems can be developed. This is fully implemented in the present study.
The closed system of static and kinematic incremental equations formulated in the local
principal stress frame is obtained and analyzed. A number of self-similar solutions of the
axially-symmetric problem is given by introducing a self-similar variable as the products of
powers of the isostatic co-ordinates. For special values of parameters involved in the self-sim
ilar solution the problem is reduced to obtaining solution of a non-linear non-autonomous
ordinary differential equation. Then this equation is numerically analyzed. The computation
of principal stresses distributions within the self-similar solutions zone is implemented.
Пространственная задача математической теории пластичности
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