Hlavácek M, Novák J
Institute of Theoretical and Applied Mechanics, Academy of Sciences of Czech Republic, Prague, Czech Republic.
J Biomech. 1995 Oct;28(10):1193-8. doi: 10.1016/0021-9290(94)00180-c.
A mixture model of synovial fluid filtration and synovial gel formation at normal approach of cartilage surfaces in the human synovial joints loaded by a compressive force has been recently presented in Parts I and II of this paper (Hlavácek, 1993, J. Biomechanics 26, 1145-1150; 1151-1160). In the model synovial fluid is taken as a mixture of two incompressible fluids (ideal and Newtonian viscous), while the biphasic model of Mow et al. (1980, J. Biomech. Engng 102, 73-84) is used for cartilage. A system of partial differential equations for the normal approach of axially symmetric cartilage surfaces in the human hip joint obtained in Part II is solved numerically for low loads. A shallow pocket-type configuration of the synovial film is formed shortly after the load application at time t = 0. For constant loads the fluid film pressure profile follows very closely that in a dry frictionless contact. To this approximation and with the exception of a close vicinity of the squeeze-film edge the flux of the ideal fluid across the synovial fluid-cartilage interface varies quadratically with the radial distance r and decreases as t-1/2 with time. The ideal fluid is forced into cartilage at the central region and out of cartilage at the low-pressure periphery of the squeezed synovial film. The maximum gel-forming concentration (the 20-fold of the original value) of the hyaluronic acid-protein macromolecular complex of the synovial fluid is reached at the film centre first, then the gel film starts spreading quickly sideways. Later, the process slows down approaching the value r/2 1/2 where r is the radius of a dry frictionless contact. The final gel-film thickness decreases very slowly with the increasing r for 0 < or = r < r/2 1/2.
本文第一部分和第二部分(Hlavácek,1993,《生物力学杂志》26卷,1145 - 1150页;1151 - 1160页)最近提出了一个关于人体滑膜关节软骨表面在压缩力作用下正常靠近时滑液过滤和滑膜凝胶形成的混合模型。在该模型中,滑液被视为两种不可压缩流体(理想流体和牛顿粘性流体)的混合物,而软骨则采用Mow等人(1980,《生物力学工程杂志》102卷,73 - 84页)的双相模型。第二部分得到的人体髋关节轴对称软骨表面正常靠近的偏微分方程组针对低载荷进行了数值求解。在t = 0时刻施加载荷后不久,就形成了一个浅袋状的滑膜结构。对于恒定载荷,流体膜压力分布与干摩擦无接触时的情况非常接近。在此近似下,除了挤压膜边缘附近区域外,理想流体穿过滑液 - 软骨界面的通量随径向距离r呈二次方变化,并随时间按t - 1/2减小。理想流体在挤压滑膜的中心区域被压入软骨,在其低压周边区域流出软骨。滑液中透明质酸 - 蛋白质大分子复合物的最大凝胶形成浓度(为初始值的20倍)首先在膜中心达到,然后凝胶膜开始迅速向侧面扩展。之后,该过程减慢,接近r/2 1/2的值,其中r是干摩擦无接触的半径。对于0≤r<r/2 1/2,最终凝胶膜厚度随r的增加而非常缓慢地减小。