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General Orthopaedics

ACETABULAR SHELL DEFORMATION AS A FUNCTION OF STIFFNESS AND BONE STRENGTH

The International Society for Technology in Arthroplasty (ISTA), 28th Annual Congress. PART 1.



Abstract

INTRODUCTION

Deformation of modular acetabular press-fit shells is of much interest for surgeons and manufacturers. Initial fixation is achieved through press-fit between shell and acetabulum with the shell mechanically deforming upon insertion. Shell deformation may disrupt the assembly process of modular systems and may adversely affect integrity and durability of the components and tribology of the bearing. The aim of the study was to show shell deformation as a function of bone and shell stiffness.

METHODS

The stiffness of the generic shells was determined using a uniaxial/ two point loading frame by applying different loads, and the change in dimension was measured by a coordinate measurement machine (CMM). Cadaver lab deformation measurements were done before and after insertion for 32 shells with 2 wall thicknesses and 11 shell sizes using the ATOS Triple Scan III (ATOS) optical system previously validated as a suitable measurement system to perform those measurements. Multiple deformation measurements per cadaver were performed by using both hip sides and stepwise increasing the reamed acetabulum by at least 1 mm, depending on sufficient residual bone stock. The under-reaming was varied between 0mm and 1mm, respectively. From the deformations, the resulting forces on the shells and bone stiffness were calculated assuming force equilibrium as well as linear-elastic material behaviour in each point at the rim of the shell.

RESULTS

Radial stiffness for shells with 3 mm wall thickness ranged between 6257 N/mm and 2920 N/mm, with 4 mm wall thickness it ranged between 14341 N/mm and 6875 N/mm. The radial shell deformation ranged between 3 µm and 187 µm. The resulting maximum radial forces acting on the shells ranged between 26 N and 916 N.

From these values, bone stiffness [N/mm] at the point of the maximum deformation has been calculated. Adding the bone stiffness and the shell stiffness using the equation for serial springs, one obtains a positive correlation between total stiffness and maximum deformation.

DISCUSSION

The measured deformation values are within the same order of magnitude previously published [Lin 2006, Squire 2006]. The large variations of resulting maximum forces exhibit the need to further investigate shell deformation using commercial shell systems. The calculated bone stiffness at the point of the maximum deformation seems to be a valid predictor for expected shell deformation, but this also needs more data. A future goal is to determine expected shell deformation from bone data as a design rational.


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