M. Jha et al., NEAR-TIP MODE-I ELASTIC FIELDS IN BIMATERIAL LAYERED SYSTEMS, International journal of solids and structures, 34(15), 1997, pp. 1849-1871
The micromorphic stress fields in the near-tip region of a Mode-I semi
-infinite crack embedded in an infinite elastic bimaterial layered sys
tem are investigated. The local and global features of the micromorphi
c stresses in the heterogeneous near-tip domain are captured through a
n approximate analytical model vis-lr-ais a two-dimensional plane stra
in finite element model. The studies are carried out within a heteroge
neous cut-out region surrounding the physical crack-tip wherein altern
ating matrix and fiber layers are positioned perpendicular to the crac
k plane. The approximate analytical model is developed by postulating
a general form of displacement field that is obtained by the superposi
tion of the applied homogenized near-tip field and a family of kinemat
ically admissible unit-cell micro-displacements. While preserving the
aggregate response of the material, these micro-displacements take int
o account the effects of material micro-structure. The results indicat
e that the microstress field in the immediate vicinity of the crack-ti
p exhibits an r(-1/2) singularity when the crack-tip is located entire
ly within the matrix phase and lies sufficiently away from the adjacen
t interfaces. The structure of the stress field in the matrix region s
urrounding the crack-tip corresponds to the universal isotropic field
dominated by the tip stress intensity factor. In the farfield region (
radial distance greater than one unit-cell thickness), the continuous
stress components sigma(xx) and sigma(xy) are found to be dominated by
the orthotropic stress intensity factor and found to be in good agree
ment with their homogeneous orthotropic counterparts. As expected, the
discontinuous stress component sigma(yy) is found to exhibit strong d
ependency on the material heterogeneity. While sigma(yy) is dominated
by the applied orthotropic stress intensity factor, it is described by
a discontinuous spatial eigen-function which has been obtained with t
he aid of the analytical approximate model. Several parameter studies
are presented and implications on the mode-I brittle fracture in layer
ed systems are discussed. (C) 1997 Elsevier Science Ltd.