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Nonlinear response of mode I crack on bimaterial interfaces

โœ Scribed by Hao Tian-hu


Publisher
Springer Netherlands
Year
1989
Tongue
English
Weight
152 KB
Volume
41
Category
Article
ISSN
1573-2673

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โœฆ Synopsis


For an incompressible body, the Cartesian coordinates x i and yi correspond, respectively, to the initial and current configuration. A plane deformation of the body is represented by the mapping yi = x i +di

(1

where d is the displacement component. The deformation gradient is

and the Jacobian determinant for incompressible body is

As in [5,6], the in-plane behavior of an incompressible material, in plane strain, is essentially governed by its response to simple shear. In particular, any plane deformation of an incompressible body can always be decomposed locally into a rigid-body rotation followed, or preceded, by a simple shear [2]. The amount of this "effective load shear" k is ~YJ ~YJ i :4TzS ,-x Ux, .j = 1.2 (4) Now let us consider the constitutive law for an incompressible, isotropic


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