Abstract

Total hip metal arthroplasty (THA) constitutes an important proportion of the standard clinical hip implant usage in Medical Physics and Biomedical Engineering. A computational nonlinear optimization is performed with two commonly metal materials in Metal-on-Metal (MoM) THA. Namely, Cast Co-Cr Alloy and Titanium. The principal result is the numerical determination of the K adimensional-constant parameter of the model. Results from a new more powerful algorithm than previous contributions, show significant improvements. Numerical standard figures for dual optimization give acceptable model-parameter values with low residuals. These results are demonstrated with 2D and 3D Graphical/Interior Optimization also. According to the findings/calculations, the standard optimized metal-model parameters are mathematically proven and verified. Mathematical consequences are obtained for model improvements and in vitro simulation methodology. The wear magnitude for in vitro determinations with these model parameter data constitute the innovation of the method. In consequence, the erosion prediction for laboratory experimental testing in THA adds valuable information to the literature. Applications lead to medical physics improvements for material/metal-THA designs.

Highlights

  • Applications lead to medical physics improvements for material/metal-total hip metal arthroplasty (THA) designs

  • There are currently three material groups widely used in total hip metal arthroplasty (THA)

  • Cast Co-Cr alloy clear that the erosion is higher−at lower values of hardness, and those stair6 intervals cor28.93 × 10 9

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Summary

Introduction

There are currently three material groups widely used in total hip metal arthroplasty (THA). The principal components of a THA are cup and head. When a polyethylene cup constitutes at least one component of the THA, the bearing is considered soft [1,2,3,4], otherwise the bearing is hard. The wear of the THA implant occurs in-between the head and cup, in erosion and abrasion biotribological phenomena. This biotribological wear-interface is based on complex biomechanical forces distribution and was presented in previous publications [1,2]

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