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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

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

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Finite element models of the hip can predict cartilage pressures consistent with<br />

experimental data when subject-specific bone and cartilage geometry are accurately<br />

represented and bones are modeled as deformable [3-5]. Most published FE models,<br />

however, do not model the complex geometry of the hip joint. Prior studies have<br />

assumed spherical geometry and neglected cartilage [9] or assumed a constant cartilage<br />

thickness [1, 10, 11]. Models that assume ideal geometry underestimate peak pressures<br />

by 60%, average pressures by 21%, and overestimate contact area by 10% [4]. When<br />

bone and cartilage geometry are reconstructed from high-resolution CT images, average<br />

pressures are within 16% and contact areas are within 21% of those measured in-vitro.<br />

However, the construction and analysis of FE models of the hip is time-intensive and<br />

computationally expensive.<br />

DEA (i.e. rigid body spring method) is a computationally efficient method for<br />

calculating cartilage stresses [6-8, 12]. Bones are modeled as rigid bodies and the<br />

cartilage surface is inferred to have thickness equal to the distance between bones,<br />

represented as an array of springs [12]. Cartilage contact stress is quantified based on<br />

the deformation of each spring. Previous DEA models have assumed concentric hip<br />

joint geometry and constant cartilage thickness. These assumptions underestimate<br />

cartilage contact stress and predict unrealistic, simplified contact patterns [4, 8]. It is<br />

possible that DEA could provide realistic predictions of cartilage contact stress if<br />

subject-specific bone and cartilage geometry were incorporated. The objectives of this<br />

study were to develop and verify a DEA model that includes subject-specific bone and<br />

cartilage geometry, and to compare DEA model predictions of cartilage contact stresses<br />

with predictions from validated FEA models.<br />

3. METHODS<br />

High resolution CT image data (512×512, 320 mm field of view, resolution<br />

0.625×0.625 mm 2 , 0.6 mm slice thickness) of a 25 year old male cadaveric hip were<br />

segmented to determine cartilage thickness and the geometry of the bone-cartilage<br />

interface for the acetabulum and femur [3]. A previously validated subject-specific<br />

FEA model provided baseline geometry (cortical bone and cartilage surfaces) for both<br />

the DEA and FEA analysis [3].<br />

3.1 Discrete Element Analysis Implementation and Verification<br />

A custom C++ program was used to perform the DEA analysis. As the DEA method<br />

requires rigid bones, both the pelvis and femur were modeled as triangulated rigid<br />

surfaces, with position dependent cartilage thickness values assigned to each node.<br />

Nodal cartilage thicknesses were computed as the distance between subject-specific<br />

cartilage and cortical bone surfaces projected along the surface normals. Cartilage was<br />

represented by a distribution of compressive springs generated in the region of the<br />

femoral head underlying the acetabulum. A spring was defined for each triangular<br />

element of the acetabulum surface in this region. One end of the spring was attached at<br />

the center of the triangle on the acetabulum. The other end was determined by<br />

projecting the first point along the acetabulum surface normal onto the femoral head.<br />

The total length of each spring accounted for the acetabular and femoral cartilage<br />

thickness as well as the joint space (Fig 1). Each spring had an initial length defined as<br />

the sum of acetabular cartilage thickness, femoral cartilage thickness, and joint space at

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