A model which allows the introduction of displacements jumps to conventiona
l finite elements is developed. The path of the discontinuity is completely
independent of the mesh structure. Unlike so-called 'embedded discontinuit
y' models, which are based on incompatible strain modes, there is no restri
ction on the type of underlying solid finite element that can be used and d
isplacement jumps are continuous across element boundaries. Using finite el
ement shape functions as partitions of unity, the displacement jump across
a crack is represented by extra degrees of freedom at existing nodes. To mo
del fracture in quasi-brittle heterogeneous materials, a cohesive crack mod
el is used. Numerical simulations illustrate the ability of the method to o
bjectively simulate fracture with unstructured meshes. Copyright (C) 2001 J
ohn Wiley & Sons, Ltd.