Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas
Knowledge on cavitation bubble size distribution, ambient radius of bubbles is of interest for many applications that include therapeutic and diagnostic medicine. It however becomes a hard quest when increasing the ultrasonic frequency, when direct observation of bubble dynamics is no longer possibl...
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doaj-0d6ee7b306d34b549614058acf640e022021-04-20T05:11:57ZengElsevierUltrasonics Sonochemistry1350-41772021-05-0173105537Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gasRachel Pflieger0Geoffrey Audiger1Sergey I. Nikitenko2Muthupandian Ashokkumar3ICSM, Univ Montpellier, CEA, CNRS, ENSCM, Marcoule, France; Corresponding author.ICSM, Univ Montpellier, CEA, CNRS, ENSCM, Marcoule, FranceICSM, Univ Montpellier, CEA, CNRS, ENSCM, Marcoule, FranceSchool of Chemistry, University of Melbourne, Melbourne, VIC 3010, AustraliaKnowledge on cavitation bubble size distribution, ambient radius of bubbles is of interest for many applications that include therapeutic and diagnostic medicine. It however becomes a hard quest when increasing the ultrasonic frequency, when direct observation of bubble dynamics is no longer possible. An indirect method based on the estimation of the bubble dissolution time under pulsed ultrasound (362 kHz) is used here under optimized conditions to derive ambient radii of cavitation bubbles in water saturated with He, Ar, Xe, O2, N2 and air: 3.0 µm for Ar, 1.2 µm for He, 3.1 µm for Xe, 2.8 µm for O2, around 1 µm for N2 and air. If the pulse on-time is increased, bubble coalescence occurs, the extent of which is rather limited for Ar but extremely high for He or N2.http://www.sciencedirect.com/science/article/pii/S1350417721000791Bubble sizePulsed ultrasoundCoalescenceSonoluminescenceHeXe |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Rachel Pflieger Geoffrey Audiger Sergey I. Nikitenko Muthupandian Ashokkumar |
spellingShingle |
Rachel Pflieger Geoffrey Audiger Sergey I. Nikitenko Muthupandian Ashokkumar Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas Ultrasonics Sonochemistry Bubble size Pulsed ultrasound Coalescence Sonoluminescence He Xe |
author_facet |
Rachel Pflieger Geoffrey Audiger Sergey I. Nikitenko Muthupandian Ashokkumar |
author_sort |
Rachel Pflieger |
title |
Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas |
title_short |
Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas |
title_full |
Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas |
title_fullStr |
Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas |
title_full_unstemmed |
Impact of bubble coalescence in the determination of bubble sizes using a pulsed US technique: Part 2 – Effect of the nature of saturating gas |
title_sort |
impact of bubble coalescence in the determination of bubble sizes using a pulsed us technique: part 2 – effect of the nature of saturating gas |
publisher |
Elsevier |
series |
Ultrasonics Sonochemistry |
issn |
1350-4177 |
publishDate |
2021-05-01 |
description |
Knowledge on cavitation bubble size distribution, ambient radius of bubbles is of interest for many applications that include therapeutic and diagnostic medicine. It however becomes a hard quest when increasing the ultrasonic frequency, when direct observation of bubble dynamics is no longer possible. An indirect method based on the estimation of the bubble dissolution time under pulsed ultrasound (362 kHz) is used here under optimized conditions to derive ambient radii of cavitation bubbles in water saturated with He, Ar, Xe, O2, N2 and air: 3.0 µm for Ar, 1.2 µm for He, 3.1 µm for Xe, 2.8 µm for O2, around 1 µm for N2 and air. If the pulse on-time is increased, bubble coalescence occurs, the extent of which is rather limited for Ar but extremely high for He or N2. |
topic |
Bubble size Pulsed ultrasound Coalescence Sonoluminescence He Xe |
url |
http://www.sciencedirect.com/science/article/pii/S1350417721000791 |
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