Computational & Technology Resources
an online resource for computational,
engineering & technology publications |
|
Civil-Comp Proceedings
ISSN 1759-3433 CCP: 79
PROCEEDINGS OF THE SEVENTH INTERNATIONAL CONFERENCE ON COMPUTATIONAL STRUCTURES TECHNOLOGY Edited by: B.H.V. Topping and C.A. Mota Soares
Paper 60
A New Damage Model based on Nonlocal Displacements A. Rodríguez-Ferran, I. Morata and A. Huerta
Laboratori de Càlcul Numèric (LaCàN), Polytechnic University of Catalunya, Barcelona, Spain , "A New Damage Model based on Nonlocal Displacements", in B.H.V. Topping, C.A. Mota Soares, (Editors), "Proceedings of the Seventh International Conference on Computational Structures Technology", Civil-Comp Press, Stirlingshire, UK, Paper 60, 2004. doi:10.4203/ccp.79.60
Keywords: nonlocal damage models, nonlocal displacements, gradient models, consistent tangent matrix, quadratic convergence.
Summary
Nonlocal damage models are used to model failure of quasi-brittle
materials [1]. Nonlocality -needed to correct the
pathological mesh-dependence exhibited by local models- can be
incorporated into the model in two different ways. In integral-type models
[2,3,4], a
nonlocal state variable is computed as the weighted average of the local
state variable in a neighbourhood of the point under consideration. In
gradient-type models [5], on the other hand, higher-order
derivatives (typically second-order) are added to the partial differential
equation that describes the evolution of the nonlocal variable. Both
approaches yield similar results and are in some cases equivalent
[6].
Apart from the state variable, other variables can be selected to incorporate nonlocality. In fact, a number of proposals can be found in the literature. Either scalar (for instance: damage) or vectorial (for instance: strain) Gauss-point quantities may be transformed into the corresponding nonlocal quantities. The existing approaches for integral-type models are compared in [7] by means of a simple 1D numerical test (bar under uniaxial tension). A new proposal is made here: to use nonlocal displacements to regularize the problem. The two versions are proposed, discussed and compared in the paper: integral-type (nonlocal displacements obtained as the weighted average of standard, local displacements), see [8], and gradient-type (nonlocal displacements obtained as the solution of a second-order partial differential equation). As discussed and illustrated by means of numerical examples, the regularization capabilities of this new model are very similar to that of the standard model. Moreover, nonlocal displacements lead to mechanically sound and computationally efficient models. For the integral-type regularization, the consistent tangent matrix is much simpler to compute than for the standard approach (nonlocal state variable). This is due to the fact that nonlocality is incorporated into the model completely "upstream" of the constitutive model (i.e. at the level of displacements, the primal unknown in the finite element analysis). Nonlocality is represented in the consistent tangent matrix by a constant matrix of geometrical nonlocal connectivity, which needs to be computed only once, at the beginning of the analysis. The need for cumbersome double loops in Gauss points of the standard approach [9] is suppressed. In the gradient approach, the boundary conditions on the regularization partial differential equation have a clear physical interpretation: nonlocal displacements must coincide with local (i.e. standard) displacements in the boundary. This contrasts favourably with the controversial issue of prescribing boundary conditions for the nonlocal state variable in standard gradient models. The expression of the consistent tangent matrix is also simpler, thanks to the linear relation between local and nonlocal displacements. This gradient-enhancement of the displacement field is a very simple way to incorporate nonlocality into a finite element code equipped with standard (i.e. local models) nonlinear capabilities. References
purchase the full-text of this paper (price £20)
go to the previous paper |
|