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Powders with zero Ohmic resistance

We substantiate the mechanism of electrical conductivity of powder consisting of dielectric nanoparticles with ionized donor centers on the surface and free electrons in the bulk. It is shown that in a powder switched to a closed dc circuit, the electric field strength vanishes due to the polarizati...

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Autor principal: Kharlamov, Vladimir F.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9581898/
https://www.ncbi.nlm.nih.gov/pubmed/36261699
http://dx.doi.org/10.1038/s41598-022-22452-1
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author Kharlamov, Vladimir F.
author_facet Kharlamov, Vladimir F.
author_sort Kharlamov, Vladimir F.
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description We substantiate the mechanism of electrical conductivity of powder consisting of dielectric nanoparticles with ionized donor centers on the surface and free electrons in the bulk. It is shown that in a powder switched to a closed dc circuit, the electric field strength vanishes due to the polarization of the powder by the source of the electromotive force. The Ohmic loss becomes impossible. The electrons of the polarized powder are in the states that correspond to the minimum of the powder energy and zero Ohmic resistance. The fulfillment of these conditions does not depend on the temperature (T = 300–500 K) and the strength of the circuit current. The electric current in the powder is maintained on account of the difference in the electrochemical potentials of electrodes that are in contact with the polarized powder.
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spelling pubmed-95818982022-10-21 Powders with zero Ohmic resistance Kharlamov, Vladimir F. Sci Rep Article We substantiate the mechanism of electrical conductivity of powder consisting of dielectric nanoparticles with ionized donor centers on the surface and free electrons in the bulk. It is shown that in a powder switched to a closed dc circuit, the electric field strength vanishes due to the polarization of the powder by the source of the electromotive force. The Ohmic loss becomes impossible. The electrons of the polarized powder are in the states that correspond to the minimum of the powder energy and zero Ohmic resistance. The fulfillment of these conditions does not depend on the temperature (T = 300–500 K) and the strength of the circuit current. The electric current in the powder is maintained on account of the difference in the electrochemical potentials of electrodes that are in contact with the polarized powder. Nature Publishing Group UK 2022-10-19 /pmc/articles/PMC9581898/ /pubmed/36261699 http://dx.doi.org/10.1038/s41598-022-22452-1 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Kharlamov, Vladimir F.
Powders with zero Ohmic resistance
title Powders with zero Ohmic resistance
title_full Powders with zero Ohmic resistance
title_fullStr Powders with zero Ohmic resistance
title_full_unstemmed Powders with zero Ohmic resistance
title_short Powders with zero Ohmic resistance
title_sort powders with zero ohmic resistance
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9581898/
https://www.ncbi.nlm.nih.gov/pubmed/36261699
http://dx.doi.org/10.1038/s41598-022-22452-1
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