Bt. Chen et al., Comparison of elastic interaction of a dislocation and a crack for four bonding conditions of the crack plane, INT J FRACT, 91(2), 1998, pp. 149-164
A comparison of elastic interaction of a dislocation and a crack for four b
onding conditions of the crack plane was made. Four cases of single crystal
line material, sliding grain boundary, perfectly bonded interface, and slid
ing interface were considered. The stress intensity factors arising from ed
ge and screw dislocations and their image forces for the above four cases w
ere compared. The stress intensity factor at a crack tip along the perfectl
y bonded interface arising from screw dislocation can be obtained from that
in a single crystalline material if the shear modulus in the single crysta
lline material is replaced by the harmonic mean of both shear moduli in the
bimaterial. The stress intensity factor at a crack tip along the sliding i
nterface arising from edge dislocation in the bimaterial can be obtained fr
om that along the sliding grain boundary in the single material if the mu/(
1 - v) in the single material is substituted by the harmonic mean of mu/(1
- v) in the bimaterial where mu and v are the shear modulus and Poisson's r
atio, respectively. The solutions of screw dislocation near a crack along t
he sliding grain boundary and sliding interface are the same as that of scr
ew dislocation and its mirror image. Generally, the effect of edge dislocat
ion for perfectly bonded interface on the crack propagation is mon pronounc
ed than that for the sliding interface. The effect of edge dislocation on t
he crack propagation is mixed mode for the cases of perfectly bonded interf
ace and single crystalline material, but mode I fracture for the cases of s
liding interface and sliding grain boundary. All curves of F-x versus dista
nce u from the dislocation at interface to the right-hand crack tip are sim
ilar to one another regardless of dislocation source for both sliding inter
face and perfectly bonded interface. The level of F-x for m = 0 is larger t
han that for m = -1.