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Predicting Peak Symmetry in Capillary Zone Electrophoresis: The Concept of the Peak Shape Diagram

机译:预测毛细管区带电泳中的峰对称性:峰形图的概念

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Electrophoretic peaks generally deviate from the symmetrical Gaussian shape that is expected when diffusion is the dominant dispersion factor. A basic understanding of the electromigrational dispersion processes which give rise to peak asymmetry shows that these effects are related to the difference in mobilities between the sample ions and the buffer electrolyte ions. There is a currently adopted rule saying that if the mobility of the buffer co-ion is higher than that of the analyte, a tailing peak is obtained, while a lower mobility of the buffer co-ion results in a fronting peak. Unfortunately, the phenomena observed in practice are frequently contradictory to these rules. This paper reveals the principles of these effects and establishes a way to proceed in explaining and predicting the peak shape in electrophoresis. Based on a mathematical model of zone migration in capillary electrophoresis, the key parameter controlling me migration dynamics is found to be the velocity slope, defined as the change in the analyte migration velocity with the analyte molar fraction at infinite analyte dilution. It is shown that the sign of the velocity slope determines the peak asymmetry (fronting or tailing) and that its magnitude relates to peak width due to electromigration dispersion. In experiments where the conversion of a fronting peak of an analyte into a tailing one is induced by changing the pH of the background electrolyte, the proposed theory successfully predicts the conversion point where the peak is symmetric. For a given background electrolyte, the model allows assessment of the symmetry and width of any analyte peak. The concept of the peak shape diagram is introduced where the velocity slope contours are plotted in a ionic mobility-pK coordinate system and its utility for fast and easy predicting of the symmetry and asymmetry of peaks as well as of their migration (detection) order is demonstrated.
机译:电泳峰通常偏离对称的高斯形状,当扩散是主要的分散因子时,电泳峰会出现。对引起峰不对称的电迁移分散过程的基本理解表明,这些影响与样品离子和缓冲电解质离子之间迁移率的差异有关。目前采用的规则是,如果缓冲剂共离子的迁移率高于分析物的迁移率,则会获得拖尾峰,而缓冲剂共离子的迁移率较低会导致前峰。不幸的是,在实践中观察到的现象经常与这些规则相矛盾。本文揭示了这些效应的原理,并建立了解释和预测电泳峰形的方法。基于毛细管电泳中区域迁移的数学模型,发现控制迁移动态的关键参数是速度斜率,定义为无限量分析物稀释时分析物迁移速度随分析物摩尔分数的变化。结果表明,速度斜率的符号决定了峰的不对称性(前部或尾部),并且其大小与电迁移分散引起的峰宽有关。在通过改变背景电解质的pH值将分析物的前峰转化为尾峰的实验中,所提出的理论成功地预测了峰对称的转化点。对于给定的背景电解质,该模型可以评估任何分析物峰的对称性和宽度。引入了峰形图的概念,其中在离子迁移率-pK坐标系中绘制了速度斜率轮廓,其用于快速轻松地预测峰的对称性和非对称性以及其迁移(检测)顺序的效用是演示。

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