Abstract
A gas-filled bubble in a liquid will generally dissolve because of diffusion of gas out of the bubble into the surrounding liquid. However, when set into motion by an acoustic field, a bubble may grow by a process called rectified diffusion. This process can counteract the effect of diffusion for values of the acoustic-pressure amplitude greater than some threshold value. This threshold has been determined by a theory that uses computed radius-time curves for bubbles pulsating nonlinearly rather than assumed infinitesimal, sinusoidal motions. For radius-time curves calculated by a digital computer, this threshold has been computed for a sequence of values of gas concentration, bubble radius, and acoustic frequency. [This work was supported by the U. S. Office of Naval Research (Code 468).]
Cite
CITATION STYLE
Eller, A., & Flynn, H. G. (1963). Rectified Diffusion during Nonlinear Pulsations of Cavitation Bubbles. The Journal of the Acoustical Society of America, 35(11_Supplement), 1906–1906. https://doi.org/10.1121/1.2142783
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