Radko S P, Chrambach A
Section on Macromolecular Analysis, National Institute of Child Health and Human Development, National Institutes of Health, Bethesda, MD 20892-1580, USA.
Electrophoresis. 1998 Oct;19(14):2423-31. doi: 10.1002/elps.1150191412.
Rigid spherical particles in the size range of 5-200 nm diameter were subjected to capillary zone electrophoresis (CZE) in semidilute solutions of uncross-linked polyacrylamide of M(r) 5, 7 and 18 x 10(6) (PA-5, -7 and -18, respectively) of varying concentrations up to 1.6% and at field strengths varying from 68 to 270 V/cm. For all particles under study, the experimental Ferguson plots, log(mobility) vs. polymer concentration, permit a linear approximation. Their slope, the retardation coefficient KR = delta log (mobility)/delta (concentration), for particles smaller than 30 nm in diameter increased with particle size in PA-5 and -7 independently of electric field strength and polymer M(r). The KR of particles of 30 nm in diameter or more was found to be independent of particle size at the lowest field strength used but to decrease with it at the higher values of field strength. The decrease was parallel but shifted to higher values of retardation when the polymer M(r) increased from 5 to 7 x 10(6). With a decreasing ratio of average mesh size of the polymer network, zeta, to particle radius, R, the approach to "continuity" of the polymeric medium (zeta/R << 1) with both increasing particle size and polymer concentration does not result in the retardation behavior expected according to the macroscopic (bulk) viscosity of the solution. These experimental observations were hypothetically interpreted in terms of a transition to a retardation mechanism comprising the formation of a polymer depletion layer near the particle surface--polymer solution interface. Peak width exhibited an overall increase with PA-7 concentration for all particles studied. For particles of 30 nm in diameter or less, the increase was steepest when the radius of the particle was approximately commensurate with zeta at a given polymer concentration. For the largest particle, 205 nm in diameter, peak broadening with polymer concentration was found to correlate linearly with peak asymmetry. CZE of the particles in PA-18 solutions revealed abnormal behavior, with both mobility and peak width remaining near-constant up to a concentration of 0.08% and sharply declining at higher concentrations. The decline of relative mobility is the same-for the entire particle size range used, while peak width declines in direct relation to particle size.
将直径在5 - 200 nm范围内的刚性球形颗粒置于毛细管区带电泳(CZE)中,所用的是不同浓度(最高达1.6%)的未交联聚丙烯酰胺(M(r)分别为5×10⁶、7×10⁶和18×10⁶,即PA - 5、PA - 7和PA - 18)的半稀释溶液,电场强度范围为68至270 V/cm。对于所有研究的颗粒,实验性的弗格森图(log(迁移率)对聚合物浓度)呈现线性近似关系。对于直径小于30 nm的颗粒,其斜率(延迟系数KR = Δlog(迁移率)/Δ(浓度))在PA - 5和PA - 7中随颗粒尺寸增加,且与电场强度和聚合物M(r)无关。发现直径为30 nm及以上的颗粒的KR在所用最低电场强度下与颗粒尺寸无关,但在较高电场强度值时随颗粒尺寸减小。当聚合物M(r)从5×10⁶增加到7×10⁶时,这种减小是平行的,但延迟值移向更高。随着聚合物网络平均网眼尺寸ζ与颗粒半径R的比值减小,随着颗粒尺寸和聚合物浓度增加,聚合物介质接近“连续性”(ζ/R << 1),但并未导致根据溶液宏观(本体)粘度预期的延迟行为。这些实验观察结果被假设性地解释为向一种延迟机制的转变,该机制包括在颗粒表面 - 聚合物溶液界面附近形成聚合物耗尽层。对于所有研究的颗粒,峰宽随PA - 7浓度总体增加。对于直径为30 nm及以下的颗粒,当在给定聚合物浓度下颗粒半径与ζ大致相当时,增加最为陡峭。对于最大的颗粒,直径为205 nm,发现峰宽随聚合物浓度的增加与峰不对称性呈线性相关。颗粒在PA - 18溶液中的CZE显示出异常行为,迁移率和峰宽在浓度达到0.08%之前几乎保持恒定,而在更高浓度时急剧下降。相对迁移率的下降在所用的整个颗粒尺寸范围内是相同的,而峰宽的下降与颗粒尺寸直接相关。