1986
DOI: 10.1017/s0022112086000460
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Bubble dynamics in a compressible liquid. Part 1. First-order theory

Abstract: The radial dynamics of a spherical bubble in a compressible liquid is studied by means of a simplified singular-perturbation method to first order in the bubble-wall Mach number. It is shown that, at this order, a one-parameter family of approximate equations for the bubble radius exists, which includes those previously derived by Herring and Keller as special cases. The relative merits of these and other equations of the family are judged by comparison with numerical results obtained from the complete partial… Show more

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Cited by 576 publications
(326 citation statements)
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“…Several assumptions are made at the outset: ͑i͒ The liquid is incompressible; ͑ii͒ the gas-vapor mixture is a perfect gas; ͑iii͒ Fourier's law for heat conduction in liquid and gas; ͑iv͒ Fick's law of mass diffusion for the noncondensible gas in the liquid and for the interdiffusion of vapor and gas inside the bubble; ͑v͒ constant transport properties, liquid density, and surface tension; ͑vi͒ constant transport properties for the gas; ͑vii͒ thermal equilibrium at the gas-liquid interface; and ͑viii͒ Henry's law at the gas-liquid interface. We note that there are alternatives to some of these assumptions, for example the first-order correction for liquid compressibility 5 and van der Waals equation of state for the gas. 6 However, we neglect these higher-order effects, since the focus of this paper is on modeling the impact of heat and mass transfer on bubble dynamics, rather than all possible competing effects.…”
Section: Full Spherical Bubble Modelmentioning
confidence: 99%
“…Several assumptions are made at the outset: ͑i͒ The liquid is incompressible; ͑ii͒ the gas-vapor mixture is a perfect gas; ͑iii͒ Fourier's law for heat conduction in liquid and gas; ͑iv͒ Fick's law of mass diffusion for the noncondensible gas in the liquid and for the interdiffusion of vapor and gas inside the bubble; ͑v͒ constant transport properties, liquid density, and surface tension; ͑vi͒ constant transport properties for the gas; ͑vii͒ thermal equilibrium at the gas-liquid interface; and ͑viii͒ Henry's law at the gas-liquid interface. We note that there are alternatives to some of these assumptions, for example the first-order correction for liquid compressibility 5 and van der Waals equation of state for the gas. 6 However, we neglect these higher-order effects, since the focus of this paper is on modeling the impact of heat and mass transfer on bubble dynamics, rather than all possible competing effects.…”
Section: Full Spherical Bubble Modelmentioning
confidence: 99%
“…Keller and Miksis [11] further considered the retarded time in the equations. Prosperetti and Lezzi [12,13] explored the connections between various models and built a more sophiscated model for bubble motion. This equation of bubble motion coupled with heat and mass transfer equation around bubbles are the main equations to be solved for bubble dynamics.…”
Section: Physical Oscillations Of Cavitation Bubblesmentioning
confidence: 99%
“…The dynamics of a single spherical gas bubble in an infinite body of compressible viscoelastic material are considered based on the Keller-Miksis equation [31][32][33] …”
Section: B Bubble Dynamics: the Keller-miksis Equationmentioning
confidence: 99%