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A finite strain discrete dislocation plasticity model

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A finite strain discrete dislocation plasticity model

Citation for published version (APA):

Irani, N., Remmers, J. J. C., & Deshpande, V. S. (2014). A finite strain discrete dislocation plasticity model.

Poster session presented at Mate Poster Award 2014 : 19th Annual Poster Contest.

Document status and date:

Published: 01/01/2014

Document Version:

Accepted manuscript including changes made at the peer-review stage

Please check the document version of this publication:

• A submitted manuscript is the version of the article upon submission and before peer-review. There can be

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Blunt Crack Tip

Figure 1: Sharp and blunt crack resemble the possibility of brittle and ductile

fracture, respectively. By using small strain theory we can only model sharp

crack tips.

Goal

Our goal is to develop a discrete dislocation (DD) framework which

is capable of capturing finite lattice rotations and shape

changes due to slip. This method gives us the tools for modelling

different phenomena such as crack tip blunting, where the lattice

rotations are not negligible (Fig.1).

A Finite Strain Discrete Dislocation

Plasticity Model

Nilgoon Irani, Joris J.C. Remmers, Vikram S. Deshpande

/ Department of Mechanical Engineering

Results

Using the new framework we were able to capture the shape

changes due to slip and finite lattice rotations. Fig. 3 and 4

compare the results obtained for a tension-compression simulation

based on small strain and finite strain assumptions respectively.

Figure 4: : Finite Strain predictions of the tensile and compressive response

of an initially rectangular specimen.

Conclusions

1) We have presented a finite strain DD formulation capable of

capturing shape deformations caused by dislocation slip.

2) Our results show that unlike in small strain DD, finite strain

effects result in a size dependent tension-compression asymmetry.

References

[1] E. van der Giessen, A. Needleman, 1995

[2] N.Irani, J.J.C. Remmers, V.S. Deshpande, 2015

Introduction

For a wide range of ductile materials, plastic deformation occurs as

a consequence of the collective motion of dislocations gliding

on slip planes. This motion may lead to finite lattice rotations.

Although the significance of lattice reorientations has long been

recognized, discrete dislocation plasticity framework has been

restricted to infinitesimal deformations.

Challenges

As the displacement field on the slip plane is not unique, the

derivatives of the displacement field and therefore the strain and

stress fields become singular. Hence when solving for these fields

we have to deal with singularities.

Method

The nonlinear finite deformation problem is solved by extending the

superposition method of Giessen and Needleman [1] and applying

a Total Lagrangian setting.

Figure 2: We must keep track of all areas which were subjected to singularity.

These areas consist of the points which were touched by dislocations

during their slip.

Figure 3: Small Strain predictions of the tensile and compressive response of

an initially rectangular specimen.

As it was mentioned the displacement field is only piecewise

continuous and therefore an iterative

finite element

procedure

which is

capable of detecting areas with singularities

is needed

(Fig. 2). At time

𝑡 = 𝑡

0

, our doamin is in its undeformed

configuaration. As we increase the loading, dislocations start to

appear and they continue to deform our domain by gliding.

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