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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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at which microdamage originates. For instance, it has been used to investigate the<br />

mechanical role of components that make up bone tissue [3].<br />

Given the technical difficulties of experimentation with miniature bone samples, as well<br />

as ethical and safety concerns, numerical simulation of mechanical experiments can<br />

complement the understanding of the response of healthy and diseased bone to<br />

mechanical loading. Finite Element Analysis (FEA) can be used to further understand<br />

how microdamage occurs and the material properties of natural bone, which in turn may<br />

improve the design of implants and artificial bone material substitutes.<br />

FEA of bone nanoindentation is used to explore the post-yield properties of bone tissue,<br />

providing an extension to the indentation modulus and hardness values that are typically<br />

reported from nanoindentation, such as constitutive modelling approaches [3-6].<br />

Recently the role of friction in such simulations has been highlighted as important in<br />

determining the post-yield response of bone tissue to indentation loading [6].<br />

Due to the high computational cost associated with three-dimensional (3D) models of<br />

nanoindentation, idealised two-dimensional (2D) axisymmetric models are often used<br />

[4, 6]. Especially as material models required to fully describe the post-yield nature of<br />

bone tissue become more complex with increased computational time to solution, an<br />

axisymmetric simplification may be desirable. However, such a 2D idealisation may not<br />

adequately capture the deformation (in particular the pile-up characteristics) of the bone<br />

tissue with an indenter that does not exhibit axial symmetry. Accordingly, the aim of<br />

this study was to compare the pile-up predicted by both axisymmetric (2D) and threedimensional<br />

(3D) models of bone nanoindentation using the three-sided pyramidal<br />

Berkovich tip, including the role of friction.<br />

3. METHODS<br />

3.1 Geometry and FE mesh<br />

Two meshes were generated to compare the prediction by 2D axisymmetric and 3D FE<br />

models of pile-up of bone undergoing nanoindentation with a Berkovich indenter.<br />

Cylindrical bone blocks of equal height and radius, 150 µm and 200 µm for the 2D and<br />

3D models respectively, were meshed with solid continuum elements. The 2D<br />

simplification employed linear 4-node reduced integration axisymmetric elements<br />

(ABAQUS CAX4R), while the 3D model contained linear 8-node reduced integration<br />

hexahedral elements (ABAQUS C3D8R). The mesh was refined at the indenter tip<br />

contact and pile-up regions, as shown in Figure 1. Due to six-fold symmetry of the<br />

Berkovich indenter, one sixth of the bone block was sufficient for the 3D model.<br />

Aiming for similar meshing characteristics, the vertical face of the 3D model was<br />

meshed corresponding to the 2D model and revolved through the bone block.<br />

Preliminary mesh sensitivity analysis showed the tip reaction force and pile-up<br />

measurements were not influenced by domain size. In each simulation, the indenter was<br />

modelled as a rigid body analytical surface. Based on Lichinchi et al. [7] an equivalent<br />

conical angle of 70.3° was used for the 2D model, while the 3D model consisted of the<br />

true Berkovich indenter half angle 65.35° (Hysitron Inc., MN, USA). Both models had a<br />

tip radius of 150 nm.

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