Exposure levels for ultrasonic cavitation in the mouse neonate.

The levels for hind limb paralysis from 1 MHz, continuous wave, unfocused ultrasound in the neonatal mouse were determined at 1 and 16 bars hydrostatic pressure and at 10 and 37 degrees C. Above a specific intensity level at each temperature, the exposure duration for paralysis of 50% of specimens exposed (t50) was found to be greater at 16 bars than at 1 bar suggesting a threshold for cavitational involvement. Using these results, the intensity thresholds for cavitation were found to be in the ranges of 120-150 W/cm2 and 53-74 W/cm2 at 10 degrees C and 37 degrees C, respectively. This temperature dependence is consistent with a cavitation mechanism. In addition, the t50 at 289 W/cm2 and 10 degrees C was measured as a function of hydrostatic pressure and showed that cavitation was suppressed at hydrostatic pressures above approximately 10 bars. This result and the intensity threshold for cavitation at 1 bar and 10 degrees C yielded similar values for the threshold negative total pressure for cavitation in the neonatal mouse.

[1]  F DUNN Physical mechanisms of the action of intense ultrasound on tissue. , 1958, American journal of physical medicine.

[2]  R. Daoust,et al.  Sensitivity to RNase treatment of ribosomes and rRNA from normal rat liver and Novikoff hepatoma. , 1982, British Journal of Cancer.

[3]  R. Apfel Acoustic cavitation: a possible consequence of biomedical uses of ultrasound. , 1982, The British journal of cancer. Supplement.

[4]  Padmakar P. Lele,et al.  Effects of Ultrasound on “Solid” Mammalian Tissues and Tumors In Vivo , 1987 .

[5]  C. J. Martin,et al.  The effects of ultrasound in vivo on mouse liver in contact with an aqueous coupling medium. , 1981, Ultrasound in medicine & biology.

[6]  R. C. Eggleton,et al.  Threshold ultrasonic dosages for structural changes in the mammalian brain. , 1970, The Journal of the Acoustical Society of America.

[7]  S. Daniels,et al.  Evidence for Acoustic Cavitation In Vivo: Thresholds for Bubble Formation with 0.75-MHz Continuous Wave and Pulsed Beams , 1986, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[8]  F Dunn,et al.  Involvement of ultrasonically induced cavitation in the production of hind limb paralysis of the mouse neonate. , 1983, The Journal of the Acoustical Society of America.

[9]  C R Hill,et al.  Ultrasonically induced cavitation in vivo. , 1982, The British journal of cancer. Supplement.

[10]  F Dunn,et al.  [Ultrasound absorption in biological media]. , 1973, Biofizika.

[11]  L. Frizzell,et al.  Threshold dosages for damage to mammalian liver by high intensity focused ultrasound , 1988, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[12]  Edwin L. Carstensen,et al.  Cavitation as a mechanism for the biological effects of ultrasound on plant roots , 1979 .

[13]  Morton W. Miller,et al.  Pulsed Enhancement of acoustic cavitation: a postulated model. , 1981, Ultrasound in medicine & biology.

[14]  R. Appel,et al.  Possibility of Microcavitation from Diagnostic Ultrasound , 1986, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[15]  E. Carstensen,et al.  Effects of ultrasound on Drosophila: III. Exposure of larvae to low-temporal-average-intensity, pulsed irradiation. , 1981, Ultrasound in medicine & biology.

[16]  F Dunn,et al.  Ultrasonic threshold dosages for the mammalian central nervous system. , 1971, IEEE transactions on bio-medical engineering.

[17]  J. Lehmann,et al.  Biologic reactions to cavitation, a consideration for ultrasonic therapy. , 1953, Archives of physical medicine and rehabilitation.

[18]  H. G. Flynn Generation of transient cavities in liquids by microsecond pulses of ultrasound , 1982 .

[19]  L. Crum,et al.  Tensile strength of water , 1979, Nature.