Batko Kornelia, Slezak-Prochazka Izabella, Slezak Andrzej
Department of Informatics for Economics, University of Economics in Katowice.
Polim Med. 2013 Jan-Mar;43(1):11-9.
The reflection coefficient of the membrane (sigma) is one of the basic parameters of the polymer membrane transport. Classical methods used to determine this parameter require intensive mixing of two solutions separated by a membrane to eliminate the effects of concentration polarization. In the real conditions, especially in biological systems, this requirement is challenging. Thus, concentration boundary layers, which are the essence of the phenomenon of concentration polarization, form on both sides of the membrane.
The main aim of this paper is to determine whether the value of reflection coefficient in a concentration polarization conditions depend on the concentration of solutions and hydrodynamic state of concentration boundary layers.
In this paper, we used the hemodialysis membrane of cellulose acetate (Nephrophan) and aqueous glucose solutions as the research materials. Formalism of nonequilibrium thermodynamics and Kedem-Katchalsky equations were our research tools.
Derived mathematical equations describe the ratio of reflection coefficients in a concentration polarization conditions (sigmaS) and in terms of homogeneity of the solutions (sigma). This ratio was calculated for the configuration in which the membrane was oriented horizontally. It was shown that each of the curves has a biffurcation point. Above this point, the value of the reflection coefficients depended on the concentration of the solution, the configuration of the membrane system and the hydrodynamic concentration boundary layers. Below this point, the system did not distinguish the gravitational directions.
on coefficient of the hemodialysis membrane in a concentration polarization condition (sigmaS) is dependent on both the solutions concentration and the hydrodynamic state of the concentration boundary layers. The value of this coefficient is the largest in the state of forced convection, lower--in natural convection state and the lowest in diffusive state. Obtained equations may be relevant to the interpretation of membrane transport processes in conditions where the assumption of homogeneity of the solution is difficult to implement
膜的反射系数(σ)是聚合物膜传输的基本参数之一。用于确定该参数的经典方法需要对被膜分隔的两种溶液进行剧烈混合,以消除浓度极化的影响。在实际情况中,尤其是在生物系统中,这一要求颇具挑战性。因此,作为浓度极化现象本质的浓度边界层会在膜的两侧形成。
本文的主要目的是确定在浓度极化条件下反射系数的值是否取决于溶液浓度和浓度边界层的流体动力学状态。
在本文中,我们使用醋酸纤维素血液透析膜(Nephrophan)和葡萄糖水溶液作为研究材料。非平衡热力学形式和凯德姆 - 卡察尔斯基方程是我们的研究工具。
推导的数学方程描述了浓度极化条件下(σS)的反射系数与溶液均匀性条件下(σ)的反射系数之比。该比值是针对膜水平放置的构型计算得出的。结果表明,每条曲线都有一个分岔点。在该点之上,反射系数的值取决于溶液浓度、膜系统构型和流体动力学浓度边界层。在该点之下,系统无法区分重力方向。
血液透析膜在浓度极化条件下的反射系数(σS)既取决于溶液浓度,也取决于浓度边界层的流体动力学状态。该系数的值在强制对流状态下最大,在自然对流状态下较低,在扩散状态下最低。所得方程可能有助于解释在难以实现溶液均匀性假设的条件下的膜传输过程。