Cirovic Srdjan
The Centre for Biomedical Engineering, University of Surrey, Guildford, Surrey GU2 7TE, UK.
J Biomech Eng. 2009 Feb;131(2):021008. doi: 10.1115/1.3005159.
The dynamics of the movement of the cerebrospinal fluid (CSF) may play an important role in the genesis of pathological neurological conditions such as syringomyelia, which is characterized by the presence of a cyst (syrinx) in the spinal cord. In order to provide sound theoretical grounds for the hypotheses that attribute the formation and growth of the syrinx to impediments to the normal movement of the CSF, it is necessary to understand various modes through which CSF pulse in the spinal column propagates. Analytical models of small-amplitude wave propagation in fluid-filled coaxial tubes, where the outer tube represents dura, the inner tube represents the spinal cord, and the fluid is the CSF, have been used to that end. However, so far, the tendency was to model one of the two tubes as rigid and to neglect the effect of finite thickness of the tube walls. The aim of this study is to extend the analysis in order to address these two potentially important issues. To that end, classical linear small-amplitude analysis of wave propagation was applied to a system consisting of coaxial tubes of finite thickness filled with inviscid incompressible fluid. General solutions to the governing equations for the case of harmonic waves in the long wave limit were replaced with the boundary conditions to yield the characteristic (dispersion) equation for the system. The four roots of the characteristic equation correspond to four modes of wave propagation, of which the first three are associated with significant motion of the CSF. For the normal range of parameters the speeds of the four modes are c(1)=13 ms, c(2)=14.7 ms, c(3)=30.3 ms, and c(4)=124.5 ms, which are well within the range of values previously reported in experimental and theoretical studies. The modes with the highest and the lowest speeds of propagation can be attributed to the dura and the spinal cord, respectively, whereas the remaining two modes involve some degree of coupling between the two. When the thickness of the spinal cord, is reduced below its normal value, the first mode becomes dominant in terms of the movement of the CSF, and its speed drops significantly. This suggests that the syrinx may be characterized by an abnormally low speed of the CSF pulse.
脑脊液(CSF)的流动动力学可能在诸如脊髓空洞症等病理性神经疾病的发生中起重要作用,脊髓空洞症的特征是脊髓中存在囊肿(空洞)。为了给将空洞的形成和生长归因于脑脊液正常流动受阻的假说提供可靠的理论依据,有必要了解脑脊液脉冲在脊柱中传播的各种模式。为此,已经使用了充液同轴管中小振幅波传播的分析模型,其中外管代表硬脑膜,内管代表脊髓,液体为脑脊液。然而,到目前为止,倾向于将两根管子中的一根建模为刚性,并忽略管壁有限厚度的影响。本研究的目的是扩展分析,以解决这两个潜在的重要问题。为此,将经典的线性小振幅波传播分析应用于由充满无粘性不可压缩流体的有限厚度同轴管组成的系统。在长波极限下谐波情况下控制方程的通解被边界条件所取代,以得到系统的特征(色散)方程。特征方程的四个根对应于四种波传播模式,其中前三种与脑脊液的显著运动有关。对于参数的正常范围,四种模式的速度分别为c(1)=13 m/s,c(2)=14.7 m/s,c(3)=30.3 m/s,和c(4)=124.5 m/s,这些都在先前实验和理论研究报告的值范围内。传播速度最高和最低的模式分别可归因于硬脑膜和脊髓,而其余两种模式涉及两者之间一定程度的耦合。当脊髓厚度减小到低于其正常值时,就脑脊液的运动而言,第一种模式变得占主导地位,并且其速度显著下降。这表明空洞可能以脑脊液脉冲速度异常低为特征。