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测量纳米颗粒的zeta电位:版本1.2

Measuring Zeta Potential of Nanoparticles: Version 1.2

作者信息

Clogston Jeffrey D., Vermilya Alison

Abstract

This protocol describes the measurement of zeta potential for nanomaterial samples in aqueous solutions. Particle surface characteristics and charge play an important role in the particle’s physical state, stability in different media, agglomeration tendencies, and interaction with biological systems. These properties are especially important for nanomaterials used in a biological context (e.g. nanomedicines). Zeta potential measurement provides an indirect measure of the net charge and as a tool to compare batch-to-batch consistency. A particle in solution with a net charge has a layer of ions (of opposite charge) strongly bound to its surface; this is referred to as the Stern layer. A second diffuse outer layer is comprised of loosely associated ions. These two layers are collectively called the electrical double layer. As the particle moves (due to gravity, kinetic energy, and/or under an applied electrical field), there exists a boundary between the ions in the diffuse layer that move with the particle and ions that remain with the bulk dispersant. The electrostatic potential at this “slipping plane” boundary is the zeta potential. In zeta potential measurements, an electrical field is applied across the sample and the movement of the particles (electrophoretic mobility) is measured by the light scattering of the particles. The Henry equation is then used to calculate the zeta potential, : where is the electrophoretic mobility, ε is the dielectric constant, is the absolute zero-shear viscosity of the medium, is the Henry function, and κ is a measure of the ratio of the particle radius to the Debye length. This assay protocol outlines the procedure for sample preparation and determination of zeta potential. Guidelines for making successful zeta potential measurements are provided, as well as a discussion of relevant standards and data analysis. Examples of zeta potential results are illustrated for 30 nm nominal size colloidal gold and a G5 PAMAM amine-terminated dendrimer.

摘要

本方案描述了水溶液中纳米材料样品的zeta电位测量方法。颗粒表面特性和电荷在颗粒的物理状态、在不同介质中的稳定性、团聚趋势以及与生物系统的相互作用中起着重要作用。这些特性对于生物环境中使用的纳米材料(如纳米药物)尤为重要。zeta电位测量提供了净电荷的间接测量方法,并作为比较批次间一致性的工具。溶液中带有净电荷的颗粒在其表面有一层强烈结合的(相反电荷的)离子层;这被称为斯特恩层。第二个扩散外层由松散结合的离子组成。这两层统称为双电层。当颗粒移动时(由于重力、动能和/或在施加的电场作用下),在与颗粒一起移动的扩散层中的离子和与大量分散剂一起保留的离子之间存在一个边界。这个“滑移面”边界处的静电电位就是zeta电位。在zeta电位测量中,在样品上施加电场,并通过颗粒的光散射测量颗粒的运动(电泳迁移率)。然后使用亨利方程计算zeta电位,:其中是电泳迁移率,ε是介电常数,是介质的绝对零剪切粘度,是亨利函数,κ是颗粒半径与德拜长度之比的量度。本检测方案概述了样品制备和zeta电位测定的程序。提供了成功进行zeta电位测量的指南,以及相关标准和数据分析的讨论。给出了标称尺寸为30 nm的胶体金和G5 PAMAM胺端基树枝状大分子的zeta电位结果示例。

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