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Application of the X-FEM to the fracture of piezoelectric materials

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Texte intégral

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Application of the X-FEM to the

fracture of piezoelectric

materials

Eric Béchet1, Matthias Scherzer2, Meinhard Kuna2 1

LPMM– CNRS UMR 7554 Université de Metz - France

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Outline

● Introduction

● Updated X-FEM formulation

– New crack tip enrichment functions

– Updated SIF computation scheme

– Use of specific preconditionner

● Convergence study ● Conclusions

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Introduction

● Goal

– Propose a updated enrichment scheme for a

cracked anisotropic piezoelectric media

– Convergence study of the method

● Energy error

● SIFS and energy release rate

– Development of a SIF evaluation scheme based

on interaction integrals specific to piezoelectric materials

– Numerical crack propagation using empirical

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Introduction

● Physical model : linear piezoelectric media,

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Introduction

● Numerical Model

– Xfem field approximation

– No remeshing

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X-FEM

● Crack represented by level-sets

– Local coodinates at the crack tip

lsn lst

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X-FEM

– Singular functions

around crack tip

– Heaviside along crack surface – Remaining dofs unenriched ● Local partition of unity enrichment

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Enrichement functions

● Enrichment functions

– Jump across the crack for displacements and

potential :

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Enrichement functions

– Crack tip functions for a

piezoelectrical setting

● Must span the

eigenfunction's space at the crack tip for displacements and potential

● Depends on the material

characteristics and the orientation

● Depends on the permeability

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Enrichement functions

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Updated enrichment scheme

“topological” Enrichment

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Updated enrichment scheme

“Geometrical” Enrichment

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Condition number

● The enrichment may lead to almost-singular

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Preconditionner

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Preconditionner

Cholesky decomposition & scaling for node k :

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Preconditionner

● Trick for handling non positive definite systems

(but blockwise positive definite)

– If the matrix A belongs to the electrostatic part:

a, b and c are negative

● we need to take the opposite matrix (which is positive

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Preconditionner

Condition number of or

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Convergence study

● Exact solution – use of complex potentials

– cf. H. Sosa, Plane problems in piezoelectric media

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Convergence study

EDx EDy Sxy Syy Potential Sxx

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Convergence study

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Convergence study

● Energy norm with respect to the internal

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Convergence study

● Energy norm

– comparison with standard

crack tip enrichment

– Infinite body with embedded

crack

– inclined material axes (30°) – PZT4 orthotropic material

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Energy error

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Energy error

● The “classical” enrichment gives almost the

same results as the specific enrichment, with less computational overhead.

● It is not clear whether different material laws

(e.g. “more” anisotropic) lead to different results

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SIFs computation

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Interaction integrals

● Same procedure used to compute interaction

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Interaction integrals

Relation between G and the K factors

– Simpler case of the isotropic elasticity well known

– The Irwin matrix depends on the material orientation

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Interaction integrals

● By using the eigenfunction set, every term in the

Irwin matrix can be determined

– for instance :

– No need of finite element support because the Irwin

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Choice of

The field describes the geometry of the integration domain S.

Two choices of integration domain with regard to h:

– Topological – Geometrical

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J error

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Conclusion & future work

● Application of the X-Fem for piezos

● The convergence study shows that the four

classical enrichment functions are enough

● Use of equivalement volume integrals to

compute the electromechanical J-integral

● Interaction integrals will be used to extract K

factors

● Auxiliary fields can also be used to compute

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Conclusion & future work

● Systematic investigations of J and the K

factors's accuracy

● Propagation laws

● Investigation for a electrically permeable

crack

● 3D extensions (esp. for the eigenfunctions

Références

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