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通过半球形超微电极上的电化学碰撞原位测量绝缘颗粒的尺寸分布和浓度

In Situ Measurement of the Size Distribution and Concentration of Insulating Particles by Electrochemical Collision on Hemispherical Ultramicroelectrodes.

作者信息

Deng Zejun, Elattar Ridha, Maroun Fouad, Renault Christophe

机构信息

Physique de la Matière Condensée, CNRS , Ecole Polytechnique , 91128 Palaiseau , France.

出版信息

Anal Chem. 2018 Nov 6;90(21):12923-12929. doi: 10.1021/acs.analchem.8b03550. Epub 2018 Oct 22.

Abstract

One of the greatest limitations in electrochemical collision/nanoimpact methods is the inability to quantify the size of colliding species due to the uneven current distribution on a disk ultramicroelectrode UME (so-called edge effect). This phenomenon arises since radial diffusion is greater at the edge than the center of the active electrode surface. One method of solving this problem is fabrication of a hemispherical UME. We describe the fabrication of a hemispherical Hg UME on a disk UME by a solution-based electrochemical method, chronocoulometry. The use of hemispherical Hg UME to detect collisions of individual amine-functionalized polystyrene beads removes the "edge effect" and enables simultaneous measurements of the concentration and the size distribution of colloids in suspension. Using finite element simulations, we deduce a quantitative relation between the distribution of current step size and the size distribution of the bead. The frequency of collision measured for a given size of bead is then converted into a concentration (in mol/L) by a quantification of the relative contributions of migration and diffusion for each size of bead. Under our experimental conditions (low concentration of supporting electrolyte), migration dominates the flux of bead. The average size of polystyrene beads of 0.5 and 1 μm radius obtained by electrochemistry and scanning electron microscopy (SEM) differs by only -8% and -9%, respectively. The total concentration of polystyrene beads of 0.5 and 1 μm radius obtained by electrochemistry is found in close agreement (<10% of error) with their nominal concentrations (25 and 100 fM).

摘要

电化学碰撞/纳米冲击方法的最大局限之一是,由于圆盘超微电极(UME)上电流分布不均(即所谓的边缘效应),无法对碰撞粒子的大小进行量化。这种现象的出现是因为在活性电极表面边缘处的径向扩散比中心处更大。解决该问题的一种方法是制造半球形UME。我们描述了通过基于溶液的电化学方法——计时库仑法,在圆盘UME上制造半球形汞UME的过程。使用半球形汞UME检测单个胺官能化聚苯乙烯珠的碰撞,消除了“边缘效应”,并能够同时测量悬浮液中胶体的浓度和尺寸分布。通过有限元模拟,我们推导出电流阶跃大小分布与珠子尺寸分布之间的定量关系。然后,通过对每种尺寸珠子迁移和扩散的相对贡献进行量化,将给定尺寸珠子的碰撞频率转换为浓度(单位为mol/L)。在我们的实验条件下(支持电解质浓度较低),迁移主导了珠子的通量。通过电化学和扫描电子显微镜(SEM)获得的半径为0.5和1μm的聚苯乙烯珠的平均尺寸差异分别仅为-8%和-9%。通过电化学获得的半径为0.5和1μm的聚苯乙烯珠的总浓度与它们的标称浓度(25和100 fM)非常吻合(误差<10%)。

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