处理过程中细胞悬浮液电导率的电变化测量

Andrew J. Fairbanks, A. Darr, Anand Vadlamani, A. Garner
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引用次数: 0

摘要

高强度电脉冲(EPs)通过在质膜上形成小孔隙来改变哺乳动物细胞的机械结构。我们可以将这些电位引起的结构变化与电学性质的变化联系起来2,3。时域介电光谱(TDDS)是一种电学表征技术,它将低强度EP应用于细胞悬浮液并测量反射信号。由此,我们可以利用双壳模型2,3提取细胞内的质膜、细胞质、核包膜和核质的电导率和介电常数。然而,TDDS使用的敏感设备禁止在高强度EP期间测量这些特性的变化。在这项研究中,我们实时测量了细胞悬浮液电导率的变化,以阐明EPs过程中的运输。我们在三种不同电导率和离子浓度的细胞介质中固定了三种不同能量密度的EP应用,脉冲持续时间分别为60和300纳秒。电导率在脉冲期间增加,表明离子从细胞向细胞外介质运动。虽然与TDDS[2]观察到的电导率增加相似,但这些测量发生在暴露后超过一分钟,这意味着扩散可能起作用,而EP期间的测量只考虑电泳。我们使用一个数学模型4,将EP诱导孔隙形成的渐近Smoluchowski表示与离子运动的Nernst-Planck模型相结合,来预测离子运动对EP参数的影响,以阐明电泳和扩散的贡献。本文将讨论ep诱导的电渗透和离子传输机制的意义。
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Measurement of Electric Modification of Cell Suspension Conductivity During Treatment
High-intensity electric pulses (EPs) alter the mechanical structure of mammalian cells by creating small pores in the plasma membrane 1. One can correlate these EP induced structural changes to changes in electrical properties 2, 3. One electrical characterization technique is time domain dielectric spectroscopy (TDDS), in which one applies low intensity EP to a cell suspension and measures the reflected signal. From this, one can extract the conductivity and permittivity of the plasma membrane, cytoplasm, nuclear envelope, and nucleoplasm in cells by using a two-shell model 2, 3. However, TDDS uses sensitive equipment that prohibits measuring the changes of these properties during a high-intensity EP. In this study, we measure the changes in cell suspension conductivity in real time to elucidate ion transport during EPs. We fix EP application at three different energy densities for three cell media of different conductivity and ion concentration and pulse durations of 60 ns and 300 ns. The conductivity increased during the pulse, indicating ion motion from the cell to the extracellular medium. While similar to the increased conductivity observed by TDDS [2], those measurements occurred greater than one minute after exposure, meaning that diffusion could contribute while the measurements during the EP would only consider electrophoresis. We use a mathematical model 4 coupling the asymptotic Smoluchowski representation of EP induced pore formation with the Nernst-Planck model for ion motion to predict ion motion for the EP parameters studied here to elucidate the contributions of electrophoresis and diffusion. The implications for the mechanisms involved in EP-induced electropermeabilization and ion transport will be discussed.
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