A computer study of rectified diffusion was made over the biomedical frequency range (1–10 MHz). Solutions of the Gilmore–Akulichev [E. Cramer, in CavitationandInhomogeneitiesinUnderwaterAcoustics, edited by W. Lauterborn (Springer, New York, 1980), pp. 54–63] formulation for bubble dynamics were combined with the Eller–Flynn [A. Eller and H. G. Flynn, J. Acoust. Soc. Am. 37, 493–503 (1965)] approach to rectified diffusion in order to calculate thresholds and growth rates. It is found that: (1) for frequencies above 1 MHz, the widely held view that small bubbles grow by rectified diffusion to ‘‘resonance size’’ and then collapse violently is true only for narrow ranges of bubbles; (2) growth rates in the low megahertz range can be quite high for medically relevant pressures, ∼20 μm/s at 1 MHz, 1 bar; (3) thresholds derived analytically are accurate for low frequencies over a wide range of bubble radii but, for high frequencies, only near the fundamental resonance radius; and (4) thresholds are quite sensitive to dissolved gas concentration at low frequencies.

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