Hits:
Date of Publication:2022-10-04
Journal:固体力学学报
Volume:38
Issue:2
Page Number:157-164
ISSN No.:0254-7805
Abstract:The cohesive zone model is widely used in fracture mechanics. When the
fracture process zone (FPZ) in front of the crack tip is too large to be
neglected,the nonlinear behavior must be considered. That is to say,in
this circumstance the linear fracture mechanics is no longer valid. In
order to take into account the nonlinear behavior in FPZ,many fracture
models have been proposed,among which,the cohesive zone model (CZM)
might be one of the simplest and has been widely used. However,there
still remain some problems in the existing numerical methods; for
instance,length of the fracture process zone cannot be obtained
accurately; dense meshes are required,etc. In order to get over these
difficulties,a new analytical singular element is proposed in the
present study and further extended into the cohesive zone model for
crack propagation problems. In this singular element,the cohesive
traction is approximately expressed in the form of polynomial expanding
though Lagrange interpolation. The special solution corresponding to
each expanding term is specified analytically. Each special solution
strictly satisfies the requirements of both differential equations of
interior domain and the corresponding traction expanding terms. The real
cohesive traction acting on the cohesive crack surface is thus expressed
in a natural and strict way. Then the special solution can be
transformed into nodal forces of the present singular element.
Assembling the stiffness matrix and nodal force into the global FEM
system,the cohesive crack problem can be analyzed. An efficient
iteration procedure is also proposed to solve the nonlinear problem.
Finally, the cohesive crack propagation under arbitrary external loading
can be simulated,and the length of FPZ, crack tip opening displacement
(CTOD) and other parameters in the cohesive crack problem can be
obtained simultaneously. The validity of the present method is
illustrated by numerical examples.
Note:新增回溯数据