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The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe
The features of stationary random processes and the small parameter expansion approach are used in this work to examine the impact of random roughness on the electromagnetic flow in cylindrical micropipes. Utilizing the perturbation method, the analytical solution until second order velocity is achi...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10673585/ https://www.ncbi.nlm.nih.gov/pubmed/38004911 http://dx.doi.org/10.3390/mi14112054 |
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author | Wang, Zhili Sun, Yanjun Jian, Yongjun |
author_facet | Wang, Zhili Sun, Yanjun Jian, Yongjun |
author_sort | Wang, Zhili |
collection | PubMed |
description | The features of stationary random processes and the small parameter expansion approach are used in this work to examine the impact of random roughness on the electromagnetic flow in cylindrical micropipes. Utilizing the perturbation method, the analytical solution until second order velocity is achieved. The analytical expression of the roughness function ζ, which is defined as the deviation of the flow rate ratio with roughness to the case having no roughness in a smooth micropipe, is obtained by integrating the spectral density. The roughness function can be taken as the functions of the Hartmann number Ha and the dimensionless wave number λ. Two special corrugated walls of micropipes, i.e., sinusoidal and triangular corrugations, are analyzed in this work. The results reveal that the magnitude of the roughness function rises as the wave number increases for the same Ha. The magnitude of the roughness function decreases as the Ha increases for a prescribed wave number. In the case of sinusoidal corrugation, as the wave number λ increases, the Hartmann number Ha decreases, and the value of ζ increases. We consider the λ ranging from 0 to 15 and the Ha ranging from 0 to 5, with ζ ranging from −2.5 to 27.5. When the λ reaches 15, and the Ha is 0, ζ reaches the maximum value of 27.5. At this point, the impact of the roughness on the flow rate reaches its maximum. Similarly, in the case of triangular corrugation, when the λ reaches 15 and the Ha is 0, ζ reaches the maximum value of 18.7. In addition, the sinusoidal corrugation has a stronger influence on the flow rate under the same values of Ha and λ compared with triangular corrugation. |
format | Online Article Text |
id | pubmed-10673585 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-106735852023-11-02 The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe Wang, Zhili Sun, Yanjun Jian, Yongjun Micromachines (Basel) Article The features of stationary random processes and the small parameter expansion approach are used in this work to examine the impact of random roughness on the electromagnetic flow in cylindrical micropipes. Utilizing the perturbation method, the analytical solution until second order velocity is achieved. The analytical expression of the roughness function ζ, which is defined as the deviation of the flow rate ratio with roughness to the case having no roughness in a smooth micropipe, is obtained by integrating the spectral density. The roughness function can be taken as the functions of the Hartmann number Ha and the dimensionless wave number λ. Two special corrugated walls of micropipes, i.e., sinusoidal and triangular corrugations, are analyzed in this work. The results reveal that the magnitude of the roughness function rises as the wave number increases for the same Ha. The magnitude of the roughness function decreases as the Ha increases for a prescribed wave number. In the case of sinusoidal corrugation, as the wave number λ increases, the Hartmann number Ha decreases, and the value of ζ increases. We consider the λ ranging from 0 to 15 and the Ha ranging from 0 to 5, with ζ ranging from −2.5 to 27.5. When the λ reaches 15, and the Ha is 0, ζ reaches the maximum value of 27.5. At this point, the impact of the roughness on the flow rate reaches its maximum. Similarly, in the case of triangular corrugation, when the λ reaches 15 and the Ha is 0, ζ reaches the maximum value of 18.7. In addition, the sinusoidal corrugation has a stronger influence on the flow rate under the same values of Ha and λ compared with triangular corrugation. MDPI 2023-11-02 /pmc/articles/PMC10673585/ /pubmed/38004911 http://dx.doi.org/10.3390/mi14112054 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Wang, Zhili Sun, Yanjun Jian, Yongjun The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title | The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title_full | The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title_fullStr | The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title_full_unstemmed | The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title_short | The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe |
title_sort | effect of random roughness on the electromagnetic flow in a micropipe |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10673585/ https://www.ncbi.nlm.nih.gov/pubmed/38004911 http://dx.doi.org/10.3390/mi14112054 |
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