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Considering the interactions between bubbles in a multi-bubble system in a liquid micro-cavity, a model of a spherical bubble cluster in a liquid cavity was developed to describe the dynamical effect of the viscoelastic medium outside the liquid cavity on the oscillation of bubbles, and the coupled equations of bubbles in the spherical cluster were obtained. Subsequently, the acoustic response characteristics of the bubbles were investigated by analyzing the radial oscillation, the stability of the non-spherical shape of bubbles and the threshold of inertial cavitation. The results showed that the confinement of the cavity and the bubble cluster promoted the suppression of bubble oscillation, however, to a certain extent, it might enhance the nonlinear properties of bubbles. According to the acoustic response curves at 1 MHz, it is found that the main resonance peaks shift left when increasing the bubble number, which means a minor resonant radius can be obtained. The nonlinear stability of bubbles in a confined environment is mainly determined by acoustic pressure amplitude and frequency, the initial radius of the bubble, and the bubble number density, while the effect of the cavity radius is enhanced with the increase of the driving pressure. There was a minimum unstable driving acoustic pressure threshold, depending on the initial radius of the bubbles, and the unstable regions were mainly located in the range of less than 4 μm. With the increase in driving acoustic frequency, the unstable region tends to decrease due to the increasing pressure threshold of instability. With the increase in bubble number density, the strip-type stable region scattered in the unstable region in the map was gradually transformed to a random patch-like distribution, which indicates that the bubble oscillation under high acoustic pressure is more sensitive to the parameters, and it is extremely easily perturbed to generate unstable oscillation and then collapse. A lower inertial cavitation threshold was obtained in the range of 1 μm ~ 4 μm of bubble equilibrium radius, and it was less affected by parameters and easier to excite inertial cavitation, whereas the threshold increased in the range greater than 4 μm. Comparing with influences of these parameters, the frequency and bubble number density were more critical on the inertial thresholds.
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Keywords:
- spherical bubble cluster /
- liquid cavity /
- cavitation bubbles /
- coupled oscillation
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[1] Kooiman K, Roovers S, Langeveld S A G, Kleven R T, Dewitte H, O'Reilly M A, Escoffre J M, Bouakaz A, Verweij M D, Hynynen K, Lentacker I, Stride E, Holland C K 2020 Ultrasound Med. Biol. 46 1296
[2] Xi F, Feng Y, Chen Q, Chen L, Liu J 2022 Front. Oncol. 12 852454
[3] Ellegala D B, Leong-Poi H, Carpenter J E, Klibanov A L, Kaul S, Shaffrey M E, Sklenar J, Lindner J R 2003 Circulation 108 336
[4] Lanza G M, Abendschein D R, Hall C S, Scott M J, Scherrer D E, Houseman A, Miller J G, Wickline S A 2000 J Am Soc Echocardiogr 13 608
[5] Lyons B, Balkaran J P R, Dunn-Lawless D, Lucian V, Keller S B, O'Reilly C S, Hu L, Rubasingham J, Nair M, Carlisle R, Stride E, Gray M, Coussios C 2023 Molecules 28
[6] Wischhusen J, Padilla F 2019 Irbm 40 10
[7] Guzman H R, McNamara A J, Nguyen D X, Prausnitz M R 2003 Ultrasound Med. Biol. 29 1211
[8] Liu Y, Yang H, Sakanishi A 2006 Biotechnol. Adv. 24 1
[9] Unnikrishnan S, Klibanov A L 2012 AJR Am J Roentgenol 199 292
[10] Villanueva F S, Jankowski R J, Klibanov S, Pina M L, Alber S M, Watkins S C, Brandenburger G H, Wagner W R 1998 Circulation 98 1
[11] Schenk H J, Steppe K, Jansen S 2015 Trends Plant Sci. 20 199
[12] Tanasawa I, Yang W-J 1970 J. Appl.Phys. 41 4526
[13] Wang Q X 2017 Physics of Fluids 29
[14] Vincent O, Marmottant P, Gonzalez-Avila S R, Ando K, Ohl C D 2014 Soft Matter 10 1455
[15] Church C C, Yang X M 2006 AIP Conf. Proc. 838 217
[16] Leonov K, Akhatov I 2021 Phys. Rev. E 104 015105
[17] Zhang T-R, Mo R-Y, Hu J, Chen S, Wang C-H, Guo J-Z 2021 Acta Phys. Sin. 70 124301 [张陶然,莫润阳,胡静,陈时,王成会,郭建中 2021 物理学报 70 124301]
[18] Zhang X-M, Wang C-H, Guo J-Z, Mo R-Y, Hu J, Chen S 2021 Acta Phys. Sin. 70 214305 [张先梅,王成会,郭建中,莫润阳,胡静,陈时 2021 物理学报 70 214305]
[19] Zhang X, Li F, Wang C, Guo J, Mo R, Hu J, Chen S, He J, Liu H 2022 Ultrason. Sonochem 84 105957
[20] Gaudron R, Murakami K, Johnsen E 2020 J. Mech. Phys. Solids 143
[21] Zilonova E M, Solovchuk M, Sheu T W H 2019 Ultrason. Sonochem 53 11
[22] Yasui K, Iida Y, Tuziuti T, Kozuka T, Towata A 2008 Phys. Rev. E Stat Nonlin Soft Matter Phys 77 016609
[23] Wang X, Chen W, Zhou M, Zhang Z, Zhang L 2022 Ultrason. Sonochem 84 105952
[24] An Y 2011 Phys. Rev. E Stat Nonlin Soft Matter Phys 83 066313
[25] Zhang W, An Y 2013 Phys. Rev. E Stat Nonlin Soft Matter Phys 87 053023
[26] Wang C-H, Mo R-Y, Hu J, Chen S 2015 Acta Phys. Sin. 64 234301 [王成会,莫润阳,胡静,陈时 2015 物理学报 64 234301]
[27] Xu L, Yao X-R, Shen Y 2024 Chin. Phys. B 33
[28] Liu R, Huang C-Y, Wu Y-R, Hu J, Mo R-Y, Wang C-H 2024 Acta Phys. Sin. 73 084303[刘睿,黄晨阳,武耀蓉,胡静,莫润阳,王成会 2024 物理学报 73 084303]
[29] Li F, Zhang X-M, Tian H, Hu J, Chen S, Wang C-H, Guo J-Z, Mo R-Y 2022 Acta Phys. Sin. 71 084303[李凡,张先梅,田华,胡静,陈时,王成会,郭建中,莫润阳 2022 物理学报 71 084303]
[30] Vincent O, Marmottant P, Quinto-Su P A, Ohl C D 2012 Phys. Rev. Lett. 108 184502
[31] Ma Y, Zhang G, Ma T 2022 Ultrason. Sonochem 84 105953
[32] Weninger K R, Camara C G, Putterman S J 2001 Phys. Rev. E Stat Nonlin Soft Matter Phys 63 016310
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