学位论文详细信息
ACL Strain During Single-Leg Jump Landing: An Experimental and Computational Investigation
anterior cruciate ligament;single leg jump landing;ACL strain;finite element analysis;in-vitro experiments;dynamic knee simulator
Polak, Annaadvisor:Chandrahsekar, Naveen ; advisor:Cronin, Duane ; affiliation1:Faculty of Engineering ; Chandrahsekar, Naveen ; Cronin, Duane ;
University of Waterloo
关键词: single leg jump landing;    Master Thesis;    anterior cruciate ligament;    finite element analysis;    in-vitro experiments;    ACL strain;    dynamic knee simulator;   
Others  :  https://uwspace.uwaterloo.ca/bitstream/10012/14339/1/Polak_Anna.pdf
瑞士|英语
来源: UWSPACE Waterloo Institutional Repository
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【 摘 要 】

The anterior cruciate ligament (ACL) is a commonly-injured ligament in the human knee joint. ACL injuryrepair is a costly procedure; however, left unrepaired, ACL injuries can lead to complications later in life.In order to understand ACL injury, metrics such as strain in the ACL are measured under various loadingconditions. A motion which has potential to cause ACL injury, a single leg jump landing, was replicatedand ACL strain was recorded. Two common approaches for this purpose are in-vitro studies involvingcadavers, and finite element (FE) modelling of the knee joint. Once ACL strain during the potentiallyinjurious motion is evaluated, it is easier to work towards potential improvements to protective orrehabilitative equipment, such as knee braces. The objective of the current study was to measure ACL strainduring a single leg jump landing using two different methods:1. In-vitro experiments involving cadavers: - ACL strain vs. time was measured with unbraced and braced cadaver knees.2. Finite element modelling of the human knee: - The finite element model was assessed using the in-vitro experiments, and can potentiallybe used to evaluate braced knee conditions in the future.The inputs for the experiments and finite element model were taken from motion capture, which was donein-vivo on two participants in a previous study. The two participants provided input kinetics and kinematicsof a single-leg jump landing. The kinematic and kinetic inputs were then applied to three cadavericspecimens using the dynamic knee simulator (DKS) at the University of Waterloo, and ACL strain relativeto the beginning of the trial was measured. The cadaver knees were also tested wearing an Össur CTiCustom knee brace, and the effect of the knee brace on relative ACL strain was measured. A finite elementmodel of the human knee joint was also investigated by extracting the right leg of an existing full humanbody model, the Global Human Body Model Consortium (GHBMC) average-sized male (M50) model, andupdating some of the tissue mechanical properties. The same boundary conditions from the experimental ivstudy were applied to the GHBMC right leg model, and relative ACL strain was calculated and comparedagainst the experimental data.The experimental maximum relative ACL strain for an unbraced full jump landing was 0.032 and 0.057 forparticipant #1 input and 0.062 for participant #2 input. The computational maximum relative ACL strainwas 0.042 for participant #1 input and 0.139 for participant #2 input. The finite element model was able toreplicate the experimental ACL strain vs. time curves reasonably well, with a mean squared error of lessthan 0.01 for all loading scenarios.The results of the unbraced vs. braced jump landing experiments showed that the knee brace had no effecton ACL strain. The mean squared error between unbraced and braced ACL strain vs. time curves was lessthan 0.0011 for all loading cases, which is a low error value when compared to strains in the range of 0.015-0.089.The jump landing finite element model is an important first step in using finite elements to predict relativeACL strain during jump landing. Future research directions include study of factors affecting ACL strain,incorporating the knee brace into the finite element model to investigate possible improvements to thebrace, and investigating the benefits of adopting a subject-specific geometry for the model.

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