Chinese Journal of Tissue Engineering Research ›› 2018, Vol. 22 ›› Issue (7): 985-990.doi: 10.3969/j.issn.2095-4344.0106
Feng Li, Wang Jun-yuan, Liu Feng, Cheng Bo
Online:2018-03-08
Published:2018-03-08
Contact:
Liu Feng, Professor, School of Mechanical Engineering, North University of China, Taiyuan 030051, Shanxi Province, China
About author:Feng Li, Master, School of Mechanical Engineering, North University of China, Taiyuan 030051, Shanxi Province, China
Supported by:the National Natural Science Foundation of China, No. 21604074
CLC Number:
Feng Li, Wang Jun-yuan, Liu Feng, Cheng Bo. Dynamic simulation of the edge load caused by the separation of the ceramic cup and femoral head [J]. Chinese Journal of Tissue Engineering Research, 2018, 22(7): 985-990.
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2.1 步态条件下股骨头-臼杯动态分离及边缘接触力 在图6中,初始分离距离代表手术安装位置误差(如图1A)。图6所示为动态仿真下股骨头与臼杯分离距离和接触力在一个稳定周期内的变化结果。当分离距离为0 mm时(髋关节负重阶段),股骨头在臼杯内部接触,接触力大小以及变化趋势与外载荷一致,接触力的两次峰值为3 000 N,与外载相同。当动态分离距离大于0 mm时(摆动阶段),外载荷迅速减小,股骨头与臼杯开始分离,产生边缘接触,当初始分离距离为4 mm时,产生的最大动态分离距离为3.4 mm。结果还显示,当人体脚后跟着地时,股骨头将从臼杯的边缘快速滑进臼窝中(在循环周期的3%-5%),该过程中接触力值快速增大,说明当股骨头从边缘滑进臼窝时,臼杯边缘容易产生应力集中。同时说明了条纹磨损的形成以及高磨损量的产生与股骨头与臼杯的边缘接触密切相关,且其主要发生在股骨头从臼杯边缘快速回到臼窝的过程中。减少股骨头与臼杯之间的边缘接触现象,可以减少接触力在臼杯边缘的集中,对假体起到一定的保护作用。 2.2 臼杯边缘接触变形验证 选取步态周期的60%(0.6 s)和80%处(0.8 s)(图6a,b分别选取了股骨头与臼杯发生边缘接触的两个瞬时位置的变形)来计算变形,图7为对比结果。如图7所示,在步态周期60%处,随着臼杯外展角的增加,赫兹接触与ADAMS接触模型所计算的臼杯边缘变形都在增大,而在步态周期80%处,随着臼杯外展角的增加,臼杯边缘变形都在减小,在不同外展角和不同接触瞬时,仿真模型与理论模型的计算值呈现出一致的变化趋势。该验证结果表明,仿真模型中的接触刚度系数设置较好地反映了理论模型的结果。"
2.3 臼杯外展角和初始分离距离对边缘负载接触的影响 图8中,随着股骨头与臼杯初始分离距离的增加,最大动态分离距离呈线性增加的趋势,最大动态分离距离均小于初始分离距离。对于一个给定的初始分离距离,最大动态分离距离随着臼杯外展角的增大而增加。对于45°臼杯外展角,当初始分离距离< 2 mm时,股骨头与臼杯不产生边缘接触。当臼杯外展角增加到55°与65°时,产生边缘接触的最小初始分离距离分别为0.7 mm和0.5 mm。上述结果说明臼杯外展角和初始分离距离是影响边缘接触的两个重要因素。 图9中,臼杯边缘产生的最大接触力随股骨头与臼杯初始分离距离增加而增大,对于一个给定的初始分离距离,最大接触力随臼杯外展角增加而增大。对于45°臼杯外展角,2-4 mm的初始分离距离,产生的边缘最大接触力为300-400 N。当臼杯外展角为55°时,对应初始分离距离0.7-4 mm,边缘最大接触力为100-600 N。当臼杯外展角增加到65°时,对应初始分离距离0.5-4 mm,边缘最大接触力为100-1 100 N。 "
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