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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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In this study, we apply a meshless algorithm in which the computational grid is built<br />

using only nodes (Fig. 1). As such meshless discretisation eliminates the need for mesh<br />

of the inter-connected elements, the problem of computational grid distortion under<br />

large strains disappears. Discontinuities (cracks) due to fragmentation are introduced by<br />

appropriate reconstruction of nodal domains of influence. We provide verification of the<br />

algorithm in terms of its ability to model discontinuities due to fragmentation in the<br />

deforming 2-D continuum and evaluate the algorithm’s performance through modelling<br />

of elongation and fragmentation of a sample of pia-arachnoid-complex tissue.<br />

3. METHODS<br />

Fig. 1 Schematic representation of<br />

meshless discretisation facilitating<br />

arbitrary distribution of nodes.<br />

3.1 Meshless algorithm for modelling of soft tissue fragmentation<br />

Basic implementation of the Meshless Total Lagrangian Explicit Dynamics (MTLED)<br />

algorithm for computing soft tissue deformations we used in this study has been<br />

described in [8]. Its key features are: 1) Moving Least-Squares (MLS) shape functions<br />

for interpolation of field variables (displacements) between the nodes; 2) A regular<br />

independent grid of integration cells for spatial integration; 3) Total Lagrangian<br />

formulation of continuum mechanics [9]; and 4) Explicit integration in time domain<br />

using central difference method.<br />

Basic implementation of the MTLED algorithm by Horton et al. [8] does not facilitate<br />

modelling of tissue fragmentation. In this study, the discontinuity in the deformation<br />

field caused by the fragmentation was introduced by modifying the shape functions to<br />

reflect the fact that nodes and integration points located on the opposite sides of the<br />

crack cannot influence each other. The alterations to the shape functions were<br />

implemented using the visibility criterion [7] in which the crack/fragmentation line (or<br />

surface in 3-D) is considered opaque when constructing the nodal domains of influence.<br />

To efficiently implement the Visibility Criterion, we used a level set function method<br />

[10, 11]. Details of our implementation of a level set method for 2-D fragmentation<br />

problems have been described in Jin et al. [12]. Therefore, only a summary is presented<br />

in Fig. 2.<br />

Fig. 2 The concept of level set function method applied in this<br />

study for implementation of visibility criterion for modelling of<br />

fragmentation induced discontinuities: The analysed domain is<br />

divided into four subdomains (A, B, C and D) according to the<br />

sign of two level set functions φ and ψ. Division into these four<br />

subdomains is used to determine the position of a point and<br />

supporting node in relation to the fragmentation (crack, notch)<br />

line L. L1 is extension of the fragmentation line. L2 is the line<br />

normal to the fragmentation line at the crack tip.

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