Biofluid Mechanics Laboratory, Department of Mechanical Engineering, University of Louisville, Louisville, KY, 40292, USA.
Faculty of Medicine, Southampton General Hospital, University of Southampton, Southampton, SO16 6YD, UK.
Fluids Barriers CNS. 2019 May 6;16(1):13. doi: 10.1186/s12987-019-0132-y.
As an alternative to advection, solute transport by shear-augmented dispersion within oscillatory cerebrospinal fluid flow was investigated in small channels representing the basement membranes located between cerebral arterial smooth muscle cells, the paraarterial space surrounding the vessel wall and in large channels modeling the spinal subarachnoid space (SSS).
Geometries were modeled as two-dimensional. Fully developed flows in the channels were modeled by the Darcy-Brinkman momentum equation and dispersion by the passive transport equation. Scaling of the enhancement of axial dispersion relative to molecular diffusion was developed for regimes of flow including quasi-steady, porous and unsteady, and for regimes of dispersion including diffusive and unsteady.
Maximum enhancement occurs when the characteristic time for lateral dispersion is matched to the cycle period. The Darcy-Brinkman model represents the porous media as a continuous flow resistance, and also imposes no-slip boundary conditions at the walls of the channel. Consequently, predicted dispersion is always reduced relative to that of a channel without porous media, except when the flow and dispersion are both unsteady.
DISCUSSION/CONCLUSIONS: In the basement membranes, flow and dispersion are both quasi-steady and enhancement of dispersion is small even if lateral dispersion is reduced by the porous media to achieve maximum enhancement. In the paraarterial space, maximum enhancement R = 73,200 has the potential to be significant. In the SSS, the dispersion is unsteady and the flow is in the transition zone between porous and unsteady. Enhancement is 5.8 times that of molecular diffusion, and grows to a maximum of 1.6E+6 when lateral dispersion is increased. The maximum enhancement produces rostral transport time in agreement with experiments.
作为平流的替代方法,在代表位于脑动脉平滑肌细胞之间的基底膜的小通道、围绕血管壁的旁腔室和模拟脊髓蛛网膜下腔(SSS)的大通道内,通过振荡脑脊液流动的剪切增强弥散来研究溶质传输。
将几何形状建模为二维。通过达西-布兰金动量方程和被动传输方程对通道中的充分发展流动进行建模。开发了相对分子扩散增强轴向弥散的标度,适用于包括准稳态、多孔和非稳态的流动和包括扩散和非稳态的弥散。
当横向弥散的特征时间与周期匹配时,最大增强发生。达西-布兰金模型将多孔介质表示为连续流动阻力,并且还在通道壁上施加无滑移边界条件。因此,与没有多孔介质的通道相比,预测的弥散总是减小,除非流动和弥散都是非稳态的。
讨论/结论:在基底膜中,流动和弥散都是准稳态的,即使通过多孔介质减小横向弥散来实现最大增强,弥散的增强也很小。在旁腔室中,最大增强 R=73200 具有显著意义。在 SSS 中,弥散是不稳定的,流动处于多孔和非稳态之间的过渡区。增强是分子扩散的 5.8 倍,当横向弥散增加时,增强最大可达 1.6E+6。最大增强产生与实验一致的颅向传输时间。