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被忽略和已知的区带畸变对毛细管无区带电泳中蛋白质分离性能的影响,特别涉及在各种缓冲液中聚丙烯酰胺涂层熔融石英毛细管中的分析。I. 理论研究。

Influence of ignored and well-known zone distortions on the separation performance of proteins in capillary free zone electrophoresis with special reference to analysis in polyacrylamide-coated fused silica capillaries in various buffers. I. Theoretical studies.

作者信息

Hjertén Stellan, Mohabbati Sheila, Westerlund Douglas

机构信息

Department of Biochemistry, Uppsala University, Biomedical Center, P.O. Box 576, SE-75123, Uppsala, Sweden.

出版信息

J Chromatogr A. 2004 Oct 22;1053(1-2):181-99.

Abstract

Distortion of the starting zone upon its electrophoretic migration toward the detection window gives rise to both symmetrical zones caused by diffusion, sedimentation in the horizontal section of the capillary and the curvature of the capillary, and asymmetrical zones having their origin in Joule heating, sedimentation in the vertical section of the capillary, pH and conductivity differences between the sample zone and the surrounding buffer, solute adsorption onto the capillary wall, and association-dissociation of complexes between the analyte and a buffer constituent or between analytes. Interestingly and importantly a theoretical study shows that moderate pH and conductivity differences as well as adsorption and all of the above interactions when they are characterized by a fast on/off kinetics do not increase the zone broadening (or only slightly), because the sharpening of one boundary of the zone is about the same as the broadening of the other boundary. In addition the peak symmetry caused by a conductivity difference is in most experiments counteracted by a pH difference. The experimentally determined plate numbers in the absence of electroosmosis exceeded one million per meter in some experiments (Part II). These plate numbers are among the highest reported [Z. Zhao, A. Malik, M.L. Lee, Anal. Chem. 65 (1993) 2747; M. Gilges, K. Kleemiss, G. Schomburg, Anal. Chem. 66 (1994) 2038; H. Wan, M. Ohman, L.G. Blomberg, J. Chromatogr. A 924 (2001) 591 (plate numbers determined in the presence of electroosmosis may be higher, although the width of the zone in the capillary may be larger) [p. 680 in S. Hjertén, Electrophoresis 11 (1990) 665]). Capillary free zone electrophoresis is perhaps the only separation method, which, under optimum conditions, gives a plate number not far from the theoretical limit. A prerequisite for this high performance is that the polyacrylamide-coated capillary is washed with 2 M HCl between the runs and stored in water over night (Part II). The difference between the experimentally determined total variance and the sum of the calculated variances originating from the width of the starting zone, longitudinal diffusion, Joule heating, sedimentation in the vertical section of the capillary, curvature of the capillary (i.e., the sum of all other variances) was in our most successful experiments about 28% of the variance of diffusion. The zone broadening, 2sigma, caused by diffusion was estimated at 0.77 mm. The total zone width (2sigma) calculated from the experimentally determined plate number was as small as 1 mm when the migration distance was 40 cm. Accordingly, the only efficient way to reduce drastically the total zone width is to decrease the analysis time and, thereby, the diffusional broadening. An important finding was that the variance originating from the loops of the capillary is not always negligible in high-performance runs. Therefore, one should employ straight capillaries and avoid CE apparatus with cartridges that require a strong curvature of the capillary, common in most commercial instruments. Mathematical formulas have been derived for the sedimentation of the solute zone, the enrichment factor, and the migration time in experiments where the solute is dissolved in a dilute running buffer. This zone sharpening method gave very narrow starting zones (0.04-0.4 mm). However, upon high dilution of the buffer the enrichment becomes so strong that part of the sample zone probably sediments out of the capillary; the almost inevitable change in pH may decrease the mobility of the proteins and, thus, cause the enrichment factor to become still lower than expected. Diffusion of the protein in the very narrow starting zone (located close to the tip of the capillary) and sometimes the thermal expansion of the buffer in the capillary contributes to additional loss of protein in the enrichment step. In some buffers, the interaction between the protein and the buffer constituents is so slow that the peaks become broad. Therefore, different types of buffers should be tested when high resolution is required. The relation sigma2 (the variance of the interaction between a protein and the buffer constituents) = constant x u (the mobility) seems to be valid for all proteins in the applied sample, at least when they have similar molecular masses. To facilitate the understanding of the progress of a free zone electrophoresis experiment, we have discussed in simple terms how the concentrations of the background electrolytes become rearranged during a run and why the difference between the mobilities of the proteins and the mobilities of the background electrolyte determines whether a peak exhibits fronting or tailing. A theoretical analysis of zone broadening in capillary zone electrophoresis, chromatography, and electrochromatography indicates that electrochromatography in homogeneous gels might be the only chromatographic technique which can compete in performance with free electrophoresis. Using an equation, valid not only for electrophoresis, but also for chromatography and centrifugation, the mobility of a concentration boundary has been calculated for the first time and was, as expected, low. Equations based on the Kohlrausch regulating function do not permit such calculations. Another regulating function (the H function) and some of its characteristics are briefly discussed. The theoretical discussions in this paper and the experimental studies in Part II show that high-performance electrophoresis deserves its prefix when the runs are designed to give minimum zone broadening. Some guidelines are given to facilitate this optimization. The plate numbers are so high that the resolution cannot be increased by more than 30% even if they approach the theoretically maximum values.

摘要

起始区在向检测窗口进行电泳迁移时发生畸变,这会产生由扩散、毛细管水平段中的沉降和毛细管曲率导致的对称区,以及由焦耳热、毛细管垂直段中的沉降、样品区与周围缓冲液之间的pH和电导率差异、溶质在毛细管壁上的吸附以及分析物与缓冲液成分之间或分析物之间络合物的缔合 - 解离引起的不对称区。有趣且重要的是,一项理论研究表明,适度的pH和电导率差异以及吸附以及上述所有具有快速开/关动力学特征的相互作用不会增加区带展宽(或仅略有增加),因为区带一个边界的锐化与另一个边界的展宽大致相同。此外,在大多数实验中,由电导率差异引起的峰对称性会被pH差异抵消。在一些实验(第二部分)中,在没有电渗的情况下实验测定的塔板数超过每米一百万。这些塔板数是已报道的最高值之一[Z. Zhao, A. Malik, M.L. Lee, Anal. Chem. 65 (1993) 2747; M. Gilges, K. Kleemiss, G. Schomburg, Anal. Chem. 66 (1994) 2038; H. Wan, M. Ohman, L.G. Blomberg, J. Chromatogr. A 924 (2001) 591(在存在电渗的情况下测定的塔板数可能更高,尽管毛细管中区带的宽度可能更大)[S. Hjertén, Electrophoresis 11 (1990) 665中的第680页]]。毛细管自由区电泳可能是唯一一种在最佳条件下塔板数接近理论极限的分离方法。实现这种高性能的一个前提是,聚丙烯酰胺涂层的毛细管在运行之间用2 M HCl冲洗,并在水中过夜储存(第二部分)。在我们最成功的实验中,实验测定的总方差与源自起始区宽度、纵向扩散、焦耳热、毛细管垂直段中的沉降、毛细管曲率(即所有其他方差之和)的计算方差之和之间的差异约为扩散方差的28%。由扩散引起的区带展宽2σ估计为0.77 mm。当迁移距离为40 cm时,根据实验测定的塔板数计算出的总区带宽度(2σ)小至1 mm。因此,大幅降低总区带宽度的唯一有效方法是减少分析时间,从而减少扩散展宽。一个重要的发现是,在高性能运行中,源自毛细管环的方差并非总是可以忽略不计。因此,应使用直管毛细管,并避免使用大多数商业仪器中常见的需要毛细管强烈弯曲的带有柱盒的CE仪器。已经推导出了溶质区沉降、富集因子和迁移时间的数学公式,这些公式适用于溶质溶解在稀运行缓冲液中的实验。这种区带锐化方法产生了非常窄的起始区(0.04 - 0.4 mm)。然而,当缓冲液高度稀释时,富集变得非常强烈,以至于部分样品区可能会从毛细管中沉降出来;几乎不可避免的pH变化可能会降低蛋白质的迁移率,从而导致富集因子变得比预期更低。蛋白质在非常窄的起始区(靠近毛细管尖端)中的扩散以及有时毛细管中缓冲液的热膨胀会导致富集步骤中蛋白质的额外损失。在某些缓冲液中,蛋白质与缓冲液成分之间的相互作用非常缓慢,以至于峰会变宽。因此,当需要高分辨率时,应测试不同类型的缓冲液。对于应用样品中的所有蛋白质,σ²(蛋白质与缓冲液成分之间相互作用的方差)=常数×u(迁移率)的关系似乎都是有效的,至少当它们具有相似的分子量时是这样。为了便于理解自由区电泳实验的过程,我们简单讨论了在运行过程中背景电解质的浓度是如何重新排列的,以及为什么蛋白质迁移率与背景电解质迁移率之间的差异决定了峰是呈现前沿还是拖尾。对毛细管区电泳、色谱和电色谱中区带展宽的理论分析表明,均匀凝胶中的电色谱可能是唯一一种在性能上可以与自由电泳竞争的色谱技术。使用一个不仅适用于电泳,也适用于色谱和离心的方程,首次计算了浓度边界的迁移率,正如预期的那样,其值很低。基于科尔劳施调节函数的方程不允许进行这样的计算。简要讨论了另一种调节函数(H函数)及其一些特性。本文的理论讨论和第二部分的实验研究表明,当运行设计为使区带展宽最小化时,高效电泳名副其实。给出了一些指导方针以促进这种优化。塔板数如此之高,以至于即使它们接近理论最大值,分辨率也无法提高超过30%。

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