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A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process

The present study treats the effects of mass transport, heat transfer and chemical reactions heat on the bubble dynamics by spanning a range of ambient bubble radii. The thermodynamic behavior of the acoustic bubble was shown for three wave frequencies, 355, 515 and 1000 kHz. The used acoustic ampli...

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Autores principales: Dehane, Aissa, Merouani, Slimane, Hamdaoui, Oualid, Alghyamah, Abdulaziz
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7944103/
https://www.ncbi.nlm.nih.gov/pubmed/33706197
http://dx.doi.org/10.1016/j.ultsonch.2021.105498
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author Dehane, Aissa
Merouani, Slimane
Hamdaoui, Oualid
Alghyamah, Abdulaziz
author_facet Dehane, Aissa
Merouani, Slimane
Hamdaoui, Oualid
Alghyamah, Abdulaziz
author_sort Dehane, Aissa
collection PubMed
description The present study treats the effects of mass transport, heat transfer and chemical reactions heat on the bubble dynamics by spanning a range of ambient bubble radii. The thermodynamic behavior of the acoustic bubble was shown for three wave frequencies, 355, 515 and 1000 kHz. The used acoustic amplitude ranges from 1 to 3 atm. It has been demonstrated that the ambient bubble radius, R(0), of the maximal response (i.e., maximal bubble temperature and pressure, T(max) and P(max)) is shifted toward lower values if the acoustic amplitude (at fixed frequency) or the ultrasonic frequency (at fixed amplitude) are increased. The range of the ambient bubble radius narrows as the ultrasonic frequency increases. Heat exchange at the bubble interface was found to be the most important mechanism within the bubble internal energy balance for acoustic amplitudes lower than 2.5 and 3 atm for ultrasonic frequencies of 355 and 515 kHz, respectively. For acoustic amplitudes greater or equal to 2.5 and 3 atm, corresponding to 355 and 515 kHz, respectively, mass transport mechanism (i.e., evaporation and condensation of water vapor) becomes dominant compared to the other mechanisms. At 1000 kHz, the mechanism of heat transfer persists to be dominant for all the used acoustic amplitudes (from 1 to 3 atm). Practically, all the above observations were maintained for bubbles at and around the optimum bubble radius, whereas no significant impact of the three energetic mechanisms was observed for bubbles of too lower and too higher values of R(0) (limits of the investigated ranges of R(0)).
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spelling pubmed-79441032021-03-16 A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process Dehane, Aissa Merouani, Slimane Hamdaoui, Oualid Alghyamah, Abdulaziz Ultrason Sonochem Original Research Article The present study treats the effects of mass transport, heat transfer and chemical reactions heat on the bubble dynamics by spanning a range of ambient bubble radii. The thermodynamic behavior of the acoustic bubble was shown for three wave frequencies, 355, 515 and 1000 kHz. The used acoustic amplitude ranges from 1 to 3 atm. It has been demonstrated that the ambient bubble radius, R(0), of the maximal response (i.e., maximal bubble temperature and pressure, T(max) and P(max)) is shifted toward lower values if the acoustic amplitude (at fixed frequency) or the ultrasonic frequency (at fixed amplitude) are increased. The range of the ambient bubble radius narrows as the ultrasonic frequency increases. Heat exchange at the bubble interface was found to be the most important mechanism within the bubble internal energy balance for acoustic amplitudes lower than 2.5 and 3 atm for ultrasonic frequencies of 355 and 515 kHz, respectively. For acoustic amplitudes greater or equal to 2.5 and 3 atm, corresponding to 355 and 515 kHz, respectively, mass transport mechanism (i.e., evaporation and condensation of water vapor) becomes dominant compared to the other mechanisms. At 1000 kHz, the mechanism of heat transfer persists to be dominant for all the used acoustic amplitudes (from 1 to 3 atm). Practically, all the above observations were maintained for bubbles at and around the optimum bubble radius, whereas no significant impact of the three energetic mechanisms was observed for bubbles of too lower and too higher values of R(0) (limits of the investigated ranges of R(0)). Elsevier 2021-02-20 /pmc/articles/PMC7944103/ /pubmed/33706197 http://dx.doi.org/10.1016/j.ultsonch.2021.105498 Text en © 2021 The Authors http://creativecommons.org/licenses/by-nc-nd/4.0/ This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Original Research Article
Dehane, Aissa
Merouani, Slimane
Hamdaoui, Oualid
Alghyamah, Abdulaziz
A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title_full A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title_fullStr A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title_full_unstemmed A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title_short A comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
title_sort comprehensive numerical analysis of heat and mass transfer phenomenons during cavitation sono-process
topic Original Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7944103/
https://www.ncbi.nlm.nih.gov/pubmed/33706197
http://dx.doi.org/10.1016/j.ultsonch.2021.105498
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