Title: Approximation of displacement and mixed formulations of solids with embedded discontinuities using the Meshless Element Free Galerkin Method
1Approximation of displacement and mixed
formulations of solids with embedded
discontinuities using the Meshless Element Free
Galerkin Method
- Felix Saucedo, Gustavo Ayala and Gelacio Juárez
2Outline
- Motivation
- Objective
- Variational formulation
- Isotropic continuum damage model
- Isotropic discrete damage model
- Approximation by Element Free Galerkin Method
- Weight functions
- Numerical integration
- Example
- Conclusions
3Motivation
- Finite element strain localization in elastic
damage - The finite element solutions are very sensitive
to mesh size and orientation. - Distortion of mesh.
Chen, Wu Belytschko 2000
4Objective
- Develop a displacement and mixed variational
formulations and approximations by a meshless
method for a solid with embedded discontinuities. - This is advance of my PhD work.
-
5Variational formulation
- The functional energy proposed by Fraeijs de
Veubeke for a continuum solid - for a solid with embedded discontinuities develop
by Juarez and Ayala
6Displacement variational formulation
- Derived formulations
- the functional with two independent fields is
given by - and for the Discrete Discontinuity approach
7Strain-Displacement mixed formulation
- Now, in this case the displacement, traction and
strain fields are considered independent - for Discrete Discontinuity approach
8Field approximation
- The independent fields for the formulations are
approximated as - Dependent field
9Approximation of the displacement formulation
- The solution to the continuum problem are
functions u and t which make P stationary. That
is for a solution to the continuum problem, the
variation is dP 0, then we have - To approximate the stationary value of the energy
functional of the displacement approach the
following matrix is obtained
10Discrete discontinuity approximation
- The first variation for Discrete Discontinuity
approach - replacing the approximation
11Lagrange multipliers
- The variational (or weak) form of the equilibrium
equation is posed as follows. Consider trial
functions and Lagrange
multipliers for all test functions
and . Then if (
Dolbow and Belytschko, 1996)
12Approximation of the mixed formulation
- In this case, the first variation
- To approximate it, the following matrix is
obtained
13Discrete discontinuity approximation
- The first variation
- To approximate it, the following matrix is
obtained
14Isotropic continuum damage model
- Free energy Helmholtz
- Damage variable
- Constitutive equation
- Law of evolution of damage
- Damage criterion
- Rule hardening
- Loading/unloading conditions
- Consistency condition
15Continuum damage model
16Isotropic discrete damage model
- Free energy Helmholtz
- Damage variable
- Constitutive equation
- Law of evolution of damage
- Damage criterion
- Rule hardening
- Loading/unloading conditions
- Consistency condition
17Discrete damage model
18Approximation by Element Free Galerkin Method
- Approximation of u(x) can be expressed as
- In order to determine a(x), a weighted discrete
error norm can be constructed as - Minimize quadratic form, leads to linear
equations for a can be written in shape function
form
19Weight function
20Numerical integration Gaussian
Background mesh
Gauss point
21How do I use EFGM?
22Example Tension bar
23Solution 1D
- Displacement d vs. load P
24Conclusions
- The presented variational formulations impose in
a natural way the essential boundary conditions
in the Meshless Method approximation. - The use of continuum damage models in Meshless
Methods does not need tracking to propagate
damage.
25Thank you