Determination of the electric field and anomalous heating caused by exponential pulses with aluminum electrodes in electroporation experiments |
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| Institution: | 1. School of Medicine, Shiraz University of Medical Sciences, Shiraz, Iran;2. Ionizing and Non-ionizing Radiation Protection Research Center (INIRPRC), Shiraz University of Medical Sciences, Shiraz, Iran;1. Photonics Research Laboratory (PRL), Department of Electronics and Communication Engineering, Indian Institute of Technology, Roorkee 247667, Uttarakhand, India;2. Photonics Research Laboratory (PRL), Department of Electronics Engineering, Indian School of Mines, Dhanbad 826004, India;1. TNlist and Department of Automation, Tsinghua University, Beijing, China;2. Centre for Signal Processing, Department of Electronic and Information Engineering, The Hong Kong Polytechnic University, Hong Kong;1. Institute of Geophysics, China Earthquake Administration, Beijing, China;2. Key Laboratory of Comprehensive and Highly Efficient Utilization of Salt Lake Resources, Qinghai Institute of Salt Lakes, Chinese Academy of Sciences, Xining, China;3. Qinghai Provincial Key Laboratory of Geology and Environment of Salt Lakes, Qinghai Institute of Salt Lakes, Chinese Academy of Sciences, Xining, China;4. Guangdong Provincial Key Laboratory of Geodynamics and Geohazards, School of Earth Sciences and Engineering, Sun Yat-Sen University, Guangzhou, China |
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| Abstract: | Electroporation is well known to depend non-linearly on the magnitude and duration of the change ΔU(t) in transmembrane voltage. In the case of cell suspension experiments, an electric field Ee(t) within the electrolyte causes ΔU(t), which is governed by both the size and shape of a cell, and also by Ee(t). It is therefore important to determine the magnitude and time dependence of the electric field to which cells are actually exposed in electroporation experiments. This can be significantly different from the nominal field En, which is calculated by using electrode voltages and geometries alone. Throughout we used single, nominally exponential pulses with time constants τpulse ranging from about 0.6 to 5 ms and found that Ee was always less than En. In order to determine the actual electric field pulse, we measured the voltage across the electrodes, the current through the cuvette, the temperature rise of the pulsing medium, and the voltage across two special electrodes placed within the cuvette. From these measurements we calculated the field strength inside the cuvette using two different methods. In addition, we compared the measured temperature rise with that expected from the electrical power dissipation. In some cases there was much larger (“anomalous”) heating, due to interfacial electrochemical heat production; for one pulsing solution Te(t) was about 30 K larger than expected. These effects are important for experiments aimed at elucidating the electroporation mechanism, comparing results obtained under different conditions, and guiding applications. |
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