Johnson E M, Berk D A, Jain R K, Deen W M
Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge 02139, USA.
Biophys J. 1996 Feb;70(2):1017-23. doi: 10.1016/S0006-3495(96)79645-5.
The diffusivities of uncharged macromolecules in gels (D) are typically lower than in free solution (D infinity), because of a combination of hydrodynamic and steric factors. To examine these factors, we measured D and D infinity for dilute solutions of several fluorescein-labeled macromolecules, using an image-based fluorescence recovery after photobleaching technique. Test macromolecules with Stokes-Einstein radii (rs) of 2.1-6.2 nm, including three globular proteins (bovine serum albumin, ovalbumin, lactalbumin) and four narrow fractions of Ficoll, were studied in agarose gels with agarose volume fractions (phi) of 0.038-0.073. The gels were characterized by measuring the hydraulic permeability of supported agarose membranes, allowing calculation of the Darcy permeability (kappa) for each gel sample. It was found that kappa, which is a measure of the intrinsic hydraulic conductance of the gel, decreased by an order of magnitude as phi was increased over the range indicated. The diffusivity ratio D/D infinity, which varied from 0.20 to 0.63, decreased with increases in rs or phi. Thus as expected, diffusional hindrances were the most severe for large macromolecules and/or relatively concentrated gels. According to a recently proposed theory for hindered diffusion through fibrous media, the diffusivity ratio is given by the product of a hydrodynamic factor (F) and a steric factor (S). The functional form is D/D infinity = F(rs/k1/2) S(f), where f = [(rs+rf)/rf]2 phi and rf is the fiber radius. Values of D/D infinity calculated from this effective medium theory, without use of adjustable parameters, were in much better agreement with the measured values than were predictions based on other approaches. The strengths and limitations of the effective medium theory for predicting diffusivities in gels are discussed.
由于流体动力学和空间位阻因素的共同作用,不带电荷的大分子在凝胶中的扩散系数(D)通常低于在自由溶液中的扩散系数(D∞)。为了研究这些因素,我们使用基于图像的光漂白后荧光恢复技术,测量了几种荧光素标记的大分子稀溶液的D和D∞。研究了斯托克斯-爱因斯坦半径(rs)为2.1 - 6.2 nm的测试大分子,包括三种球状蛋白质(牛血清白蛋白、卵清蛋白、乳白蛋白)和四个窄级分的聚蔗糖,它们在琼脂糖体积分数(phi)为0.038 - 0.073的琼脂糖凝胶中进行研究。通过测量支撑琼脂糖膜的水力渗透率来表征凝胶,从而计算每个凝胶样品的达西渗透率(kappa)。结果发现,kappa作为凝胶固有水力传导率的度量,在所示范围内随着phi的增加下降了一个数量级。扩散系数比D/D∞在0.20至0.63之间变化,随着rs或phi的增加而降低。因此,正如预期的那样,对于大分子和/或相对浓缩的凝胶,扩散阻碍最为严重。根据最近提出的关于通过纤维介质的受阻扩散理论,扩散系数比由流体动力学因子(F)和空间位阻因子(S)的乘积给出。函数形式为D/D∞ = F(rs/k1/2) S(f),其中f = [(rs + rf)/rf]2 phi,rf是纤维半径。由这种有效介质理论计算得到的D/D∞值,无需使用可调参数,与测量值的一致性比基于其他方法的预测要好得多。讨论了有效介质理论在预测凝胶中扩散系数方面的优势和局限性。