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...

Full description

Bibliographic Details
Main Authors: Zhili Wang, Yanjun Sun, Yongjun Jian
Format: Article
Language:English
Published: MDPI AG 2023-11-01
Series:Micromachines
Subjects:
Online Access:https://www.mdpi.com/2072-666X/14/11/2054
_version_ 1797458400792018944
author Zhili Wang
Yanjun Sun
Yongjun Jian
author_facet Zhili Wang
Yanjun Sun
Yongjun Jian
author_sort Zhili Wang
collection DOAJ
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 <i>ζ</i>, 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 <i>Ha</i> and the dimensionless wave number <i>λ</i>. 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 <i>Ha</i> increases for a prescribed wave number. In the case of sinusoidal corrugation, as the wave number <i>λ</i> increases, the Hartmann number <i>Ha</i> decreases, and the value of <i>ζ</i> increases. We consider the <i>λ</i> ranging from 0 to 15 and the <i>Ha</i> ranging from 0 to 5, with <i>ζ</i> ranging from −2.5 to 27.5. When the <i>λ</i> reaches 15, and the <i>Ha</i> is 0, <i>ζ</i> 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 <i>λ</i> reaches 15 and the <i>Ha</i> is 0, <i>ζ</i> 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 <i>Ha</i> and <i>λ</i> compared with triangular corrugation.
first_indexed 2024-03-09T16:36:34Z
format Article
id doaj.art-c6343f3e6c374f319fe6c06c841ca041
institution Directory Open Access Journal
issn 2072-666X
language English
last_indexed 2024-03-09T16:36:34Z
publishDate 2023-11-01
publisher MDPI AG
record_format Article
series Micromachines
spelling doaj.art-c6343f3e6c374f319fe6c06c841ca0412023-11-24T14:56:23ZengMDPI AGMicromachines2072-666X2023-11-011411205410.3390/mi14112054The Effect of Random Roughness on the Electromagnetic Flow in a MicropipeZhili Wang0Yanjun Sun1Yongjun Jian2School of Mathematical Science, Inner Mongolia University, Hohhot 010021, ChinaSchool of Mathematical Science, Inner Mongolia University, Hohhot 010021, ChinaSchool of Mathematical Science, Inner Mongolia University, Hohhot 010021, ChinaThe 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 <i>ζ</i>, 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 <i>Ha</i> and the dimensionless wave number <i>λ</i>. 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 <i>Ha</i> increases for a prescribed wave number. In the case of sinusoidal corrugation, as the wave number <i>λ</i> increases, the Hartmann number <i>Ha</i> decreases, and the value of <i>ζ</i> increases. We consider the <i>λ</i> ranging from 0 to 15 and the <i>Ha</i> ranging from 0 to 5, with <i>ζ</i> ranging from −2.5 to 27.5. When the <i>λ</i> reaches 15, and the <i>Ha</i> is 0, <i>ζ</i> 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 <i>λ</i> reaches 15 and the <i>Ha</i> is 0, <i>ζ</i> 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 <i>Ha</i> and <i>λ</i> compared with triangular corrugation.https://www.mdpi.com/2072-666X/14/11/2054random roughnesselectromagnetic flowroughness functionmicropipe
spellingShingle Zhili Wang
Yanjun Sun
Yongjun Jian
The Effect of Random Roughness on the Electromagnetic Flow in a Micropipe
Micromachines
random roughness
electromagnetic flow
roughness function
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 random roughness
electromagnetic flow
roughness function
micropipe
url https://www.mdpi.com/2072-666X/14/11/2054
work_keys_str_mv AT zhiliwang theeffectofrandomroughnessontheelectromagneticflowinamicropipe
AT yanjunsun theeffectofrandomroughnessontheelectromagneticflowinamicropipe
AT yongjunjian theeffectofrandomroughnessontheelectromagneticflowinamicropipe
AT zhiliwang effectofrandomroughnessontheelectromagneticflowinamicropipe
AT yanjunsun effectofrandomroughnessontheelectromagneticflowinamicropipe
AT yongjunjian effectofrandomroughnessontheelectromagneticflowinamicropipe