Abstract

The present paper deals with plane strain deformation of incompressible polymers that obey quite a general pressure-dependent yield criterion. In general, the system of equations can be hyperbolic, parabolic, or elliptic. However, attention is concentrated on the hyperbolic regime and on the behavior of solutions near frictional interfaces, assuming that the regime of sliding occurs only if the friction surface coincides with an envelope of stress characteristics. The main reason for studying the behavior of solutions in the vicinity of envelopes of characteristics is that the solution cannot be extended beyond the envelope. This research is also motivated by available results in metal plasticity that the velocity field is singular near envelopes of characteristics (some space derivatives of velocity components approach infinity). In contrast to metal plasticity, it is shown that in the case of the material models adopted, all derivatives of velocity components are bounded but some derivatives of stress components approach infinity near the envelopes of stress characteristics. The exact asymptotic expansion of stress components is found. It is believed that this result is useful for developing numerical codes that should account for the singular behavior of the stress field.

Highlights

  • Qualitative behavior of solutions in the vicinity of interfaces between plastic material and rigid solids essentially depends on the constitutive equations chosen

  • The friction stress is determined from the solution of a boundary value problem, and its magnitude is controlled by other boundary conditions

  • The solution is singular if the interface between plastic material and rigid solids coincides with an envelope of stress characteristics

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Summary

Introduction

Qualitative behavior of solutions in the vicinity of interfaces between plastic material and rigid solids essentially depends on the constitutive equations chosen. A less obvious case is associated with the regime of sticking at the interface between plastic material and rigid solids In this case, the friction stress is determined from the solution of a boundary value problem, and its magnitude is controlled by other boundary conditions. The quadratic invariant of the strain-rate tensor can approach infinity near the friction surface This feature of solution behavior has been demonstrated in [8] for rigid perfectly-plastic material and in [9,10] for viscoplastic material with a saturation stress. Henceforward, attention is concentrated on the hyperbolic regime In this case, the solution is singular if the interface between plastic material and rigid solids coincides with an envelope of stress characteristics. By analogy to rate-dependent models of pressure-independent plasticity [9,10], it is reasonable to expect that singular asymptotic solutions may appear in the case of vanishing viscosity

Material Models
Cartesian
Characteristics and Characteristic Relations
Hgsumming sin 2ω
Orientation
Asymptotic Behavior of Solutions near Envelopes of Characteristics
Conclusions
Full Text
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