scholarly journals Chaotic characteristics of gas bubble motion in acoustic field

2011 ◽  
Vol 60 (10) ◽  
pp. 104302
Author(s):  
Shen Zhuang-Zhi ◽  
Lin Shu-Yu
2018 ◽  
Vol 40 ◽  
pp. 480-487 ◽  
Author(s):  
Xiaojian Ma ◽  
Tianyu Xing ◽  
Biao Huang ◽  
Qiuhe Li ◽  
Yifei Yang

2019 ◽  
Vol 283 ◽  
pp. 06002
Author(s):  
Yan Ma ◽  
Tao Ma ◽  
Feiyan Zhao

The exact solution of a gas bubble’ volume was obtained based on volume oscillation of a gas bubble. The volume pulsation, acoustic impedance, scattering pressure of a gas bubble, acoustical power of scattering and acoustical scattering cross section of a single bubble are researched in a small amplitude acoustic field. The results show that a big bubble oscillates more violently than that of a small bubble in a weak acoustic field if the linear resonance does not happen. The occurrence of a linear resonance response of a single bubble leads to the volume oscillation and the scattering ability of a gas bubble become stronger. Additionally, the scattering cross section does not depend on the driving pressure. The amplitude of scattering pressure of a big bubble can reach the magnitude compared to the driving pressure when the resonance response occurs.


1975 ◽  
Vol 28 (4) ◽  
pp. 415-418
Author(s):  
L. E. Kolesnikov ◽  
V. V. Sobolev
Keyword(s):  

2014 ◽  
Vol 07 (06) ◽  
pp. 1450072 ◽  
Author(s):  
S. A. Mohammadein ◽  
K. G. Mohamed

This paper presents formulae and explanation about the growth of a convective gas bubble in the blood and other tissues of divers who surface too quickly, concentration distribution around the growing bubble is also presented. The formulae are valid all over the growth stages, i.e. under variable ambient pressure while the diver is ascending, and under constant ambient pressure at diving stops or at sea level. The mathematical model is solved analytically by using the method of combined variables. The growth process is affected by tissue diffusivity, concentration constant and the initial void fraction, which is the dominant parameter. Results show that, the time of the complete growth, in the convective growth model, is shorter than those earlier presented by Mohammadein and Mohamed [Concentration distribution around a growing gas bubble in tissue, Math. Biosci.225(1) (2010) 11–17] and Srinivasan et al. [Mathematical models of diffusion-limited gas bubble dynamics in tissue, J. Appl. Physiol.86 (1999) 732–741] for the growth of a stationary gas bubble, this explains the effect of bubble motion on consuming the oversaturated dissolved gas from the tissue into growing bubble which leads to increment in the growth rate to be more than those presented in the previous stationary models.


2008 ◽  
Vol 190 (2) ◽  
pp. 294-299 ◽  
Author(s):  
Franklin Liu ◽  
Carlos Cuevas ◽  
Albert A. Moss ◽  
Orpheus Kolokythas ◽  
Theodore J. Dubinsky ◽  
...  

2008 ◽  
Vol 78 (3) ◽  
Author(s):  
Karthik Mukundakrishnan ◽  
Portonovo S. Ayyaswamy ◽  
David M. Eckmann

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