Mathias R T
Biophys J. 1985 Jun;47(6):823-36. doi: 10.1016/S0006-3495(85)83986-2.
The relationship between epithelial fluid transport, standing osmotic gradients, and standing hydrostatic pressure gradients has been investigated using a perturbation expansion of the governing equations. The assumptions used in the expansion are: (a) the volume of lateral intercellular space per unit volume of epithelium is small; (b) the membrane osmotic permeability is much larger than the solute permeability. We find that the rate of fluid reabsorption is set by the rate of active solute transport across lateral membranes. The fluid that crosses the lateral membranes and enters the intercellular cleft is driven longitudinally by small gradients in hydrostatic pressure. The small hydrostatic pressure in the intercellular space is capable of causing significant transmembrane fluid movement, however, the transmembrane effect is countered by the presence of a small standing osmotic gradient. Longitudinal hydrostatic and osmotic gradients balance such that their combined effect on transmembrane fluid flow is zero, whereas longitudinal flow is driven by the hydrostatic gradient. Because of this balance, standing gradients within intercellular clefts are effectively uncoupled from the rate of fluid reabsorption, which is driven by small, localized osmotic gradients within the cells. Water enters the cells across apical membranes and leaves across the lateral intercellular membranes. Fluid that enters the intercellular clefts can, in principle, exit either the basal end or be secreted from the apical end through tight junctions. Fluid flow through tight junctions is shown to depend on a dimensionless parameter, which scales the resistance to solute flow of the entire cleft relative to that of the junction. Estimates of the value of this parameter suggest that an electrically leaky epithelium may be effectively a tight epithelium in regard to fluid flow.
利用控制方程的微扰展开研究了上皮细胞液体转运、静息渗透梯度和静息静水压力梯度之间的关系。展开过程中使用的假设为:(a) 单位上皮细胞体积的侧向细胞间隙体积较小;(b) 膜的渗透渗透率远大于溶质渗透率。我们发现液体重吸收速率由跨侧向膜的主动溶质转运速率决定。穿过侧向膜进入细胞间隙的液体由静水压力的微小梯度纵向驱动。细胞间隙中的小静水压力能够引起显著的跨膜液体流动,然而,跨膜效应被小的静息渗透梯度抵消。纵向静水压力和渗透梯度相互平衡,使得它们对跨膜液体流动的综合影响为零,而纵向流动由静水压力梯度驱动。由于这种平衡,细胞间隙内的静息梯度实际上与由细胞内小的局部渗透梯度驱动的液体重吸收速率解耦。水通过顶端膜进入细胞,并通过侧向细胞间膜离开。进入细胞间隙的液体原则上可以从基底端流出,或者通过紧密连接从顶端分泌。通过紧密连接的液体流动取决于一个无量纲参数,该参数衡量整个间隙相对于连接处溶质流动的阻力。对该参数值的估计表明,就液体流动而言,电渗漏上皮可能实际上是紧密上皮。