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A primary current distribution model of a novel micro-electroporation channel configuration
Traditional macro and micro-electroporation devices utilize facing electrodes, which generate electric fields inversely proportional to their separation distance. Although the separation distances in micro-electroporation devices are significantly smaller than those in macro-electroporation devices,...
Autores principales: | , |
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Formato: | Texto |
Lenguaje: | English |
Publicado: |
Springer US
2010
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2916117/ https://www.ncbi.nlm.nih.gov/pubmed/20532636 http://dx.doi.org/10.1007/s10544-010-9437-y |
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author | Troszak, Gregory D. Rubinsky, Boris |
author_facet | Troszak, Gregory D. Rubinsky, Boris |
author_sort | Troszak, Gregory D. |
collection | PubMed |
description | Traditional macro and micro-electroporation devices utilize facing electrodes, which generate electric fields inversely proportional to their separation distance. Although the separation distances in micro-electroporation devices are significantly smaller than those in macro-electroporation devices, they are limited by cell size. Because of this, significant potential differences are required to induce electroporation. These potential differences are often large enough to cause water electrolysis, resulting in electrode depletion and bubble formation, both of which adversely affect the electroporation process. Here, we present a theoretical study of a novel micro-electroporation channel composed of an electrolyte flowing over a series of adjacent electrodes separated by infinitesimally small insulators. Application of a small, non-electrolysis inducing potential difference between the adjacent electrodes results in radially-varying electric fields that emanate from these insulators, causing cells flowing through the channel to experience a pulsed electric field. This eliminates the need for a pulse generator, making a minimal power source (such as a battery) the only electrical equipment that is needed. A non-dimensional primary current distribution model of the novel micro-electroporation channel shows that decreasing the channel height results in an exponential increase in the electric field magnitude, and that cells experience exponentially greater electric field magnitudes the closer they are to the channel walls. Finally, dimensional primary current distribution models of two potential applications, water sterilization and cell transfection, demonstrate the practical feasibility of the novel micro-electroporation channel. |
format | Text |
id | pubmed-2916117 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2010 |
publisher | Springer US |
record_format | MEDLINE/PubMed |
spelling | pubmed-29161172010-08-20 A primary current distribution model of a novel micro-electroporation channel configuration Troszak, Gregory D. Rubinsky, Boris Biomed Microdevices Article Traditional macro and micro-electroporation devices utilize facing electrodes, which generate electric fields inversely proportional to their separation distance. Although the separation distances in micro-electroporation devices are significantly smaller than those in macro-electroporation devices, they are limited by cell size. Because of this, significant potential differences are required to induce electroporation. These potential differences are often large enough to cause water electrolysis, resulting in electrode depletion and bubble formation, both of which adversely affect the electroporation process. Here, we present a theoretical study of a novel micro-electroporation channel composed of an electrolyte flowing over a series of adjacent electrodes separated by infinitesimally small insulators. Application of a small, non-electrolysis inducing potential difference between the adjacent electrodes results in radially-varying electric fields that emanate from these insulators, causing cells flowing through the channel to experience a pulsed electric field. This eliminates the need for a pulse generator, making a minimal power source (such as a battery) the only electrical equipment that is needed. A non-dimensional primary current distribution model of the novel micro-electroporation channel shows that decreasing the channel height results in an exponential increase in the electric field magnitude, and that cells experience exponentially greater electric field magnitudes the closer they are to the channel walls. Finally, dimensional primary current distribution models of two potential applications, water sterilization and cell transfection, demonstrate the practical feasibility of the novel micro-electroporation channel. Springer US 2010-06-08 2010 /pmc/articles/PMC2916117/ /pubmed/20532636 http://dx.doi.org/10.1007/s10544-010-9437-y Text en © The Author(s) 2010 https://creativecommons.org/licenses/by-nc/4.0/ This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited. |
spellingShingle | Article Troszak, Gregory D. Rubinsky, Boris A primary current distribution model of a novel micro-electroporation channel configuration |
title | A primary current distribution model of a novel micro-electroporation channel configuration |
title_full | A primary current distribution model of a novel micro-electroporation channel configuration |
title_fullStr | A primary current distribution model of a novel micro-electroporation channel configuration |
title_full_unstemmed | A primary current distribution model of a novel micro-electroporation channel configuration |
title_short | A primary current distribution model of a novel micro-electroporation channel configuration |
title_sort | primary current distribution model of a novel micro-electroporation channel configuration |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2916117/ https://www.ncbi.nlm.nih.gov/pubmed/20532636 http://dx.doi.org/10.1007/s10544-010-9437-y |
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