Ultrasonic atomization of tissue and its role in tissue fractionation by high intensity focused ultrasound

Atomization and fountain formation is a well-known phenomenon that occurs when a focused ultrasound wave in liquid encounters an air interface. High intensity focused ultrasound (HIFU) has been shown to fractionate a tissue into submicron-sized fragments in a process termed boiling histotripsy, wherein the focused ultrasound wave superheats the tissue at the focus, producing a millimetre-sized boiling or vapour bubble in several milliseconds. Yet the question of how this millimetre-sized boiling bubble creates submicron-sized tissue fragments remains. The hypothesis of this work is that the tissue can behave as a liquid such that it atomizes and forms a fountain within the vapour bubble produced in boiling histotripsy. We describe an experiment, in which a 2 MHz HIFU transducer (maximum in situ intensity of 24 000 W cm−2) was aligned with an air–tissue interface meant to simulate the boiling bubble. Atomization and fountain formation was observed with high-speed photography and resulted in tissue erosion. Histological examination of the atomized tissue showed whole and fragmented cells and nuclei. Air–liquid interfaces were also filmed. Our conclusion was that HIFU can fountain and atomize tissue. Although this process does not entirely mimic what was observed in liquids, it does explain many aspects of tissue fractionation in boiling histotripsy.

[1]  Leonid R Gavrilov,et al.  The role of acoustic nonlinearity in tissue heating behind a rib cage using a high-intensity focused ultrasound phased array , 2013, Physics in medicine and biology.

[2]  C. Cain,et al.  An efficient treatment strategy for histotripsy by removing cavitation memory. , 2012, Ultrasound in medicine & biology.

[3]  Lawrence A Crum,et al.  Controlled tissue emulsification produced by high intensity focused ultrasound shock waves and millisecond boiling. , 2011, The Journal of the Acoustical Society of America.

[4]  Zhen Xu,et al.  Cavitation clouds created by shock scattering from bubbles during histotripsy. , 2011, The Journal of the Acoustical Society of America.

[5]  F. Starr,et al.  In vivo tissue emulsification using millisecond boiling induced by high intensity focused ultrasound. , 2011 .

[6]  L. Crum,et al.  Histological and biochemical analysis of emulsified lesions in tissue induced by high intensity focused ultrasound. , 2011 .

[7]  C. Cain,et al.  Histotripsy fractionation of prostate tissue: local effects and systemic response in a canine model. , 2011, The Journal of urology.

[8]  L. Crum,et al.  A derating method for therapeutic applications of high intensity focused ultrasound , 2010, Acoustical physics.

[9]  L. Crum,et al.  Tissue Erosion Using Shock Wave Heating and Millisecond Boiling in HIFU Fields , 2010 .

[10]  Lawrence A Crum,et al.  Shock-induced heating and millisecond boiling in gels and tissue due to high intensity focused ultrasound. , 2010, Ultrasound in medicine & biology.

[11]  C. Cain,et al.  Histotripsy of the prostate: dose effects in a chronic canine model. , 2009, Urology.

[12]  Lawrence A Crum,et al.  Acoustic characterization of high intensity focused ultrasound fields: a combined measurement and modeling approach. , 2008, The Journal of the Acoustical Society of America.

[13]  W. Phillips,et al.  On the impulsive generation of drops at the interface of two inviscid fluids , 2008, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[14]  C. Cain,et al.  Histotripsy of rabbit renal tissue in vivo: temporal histologic trends. , 2007, Journal of endourology.

[15]  W. Phillips,et al.  On impulsively generated inviscid axisymmetric surface jets, waves and drops , 2007, Journal of Fluid Mechanics.

[16]  C. Holland,et al.  Acousto-mechanical and thermal properties of clotted blood. , 2005, The Journal of the Acoustical Society of America.

[17]  L. Crum,et al.  Physical mechanisms of the therapeutic effect of ultrasound (a review) , 2003 .

[18]  Félix Barreras,et al.  Transient high-frequency ultrasonic water atomization , 2002 .

[19]  Gail ter Haar,et al.  High intensity ultrasound. , 2001 .

[20]  K Hynynen,et al.  The feasibility of using focused ultrasound for transmyocardial revascularization. , 1998, Ultrasound in medicine & biology.

[21]  J.N. Antonevich,et al.  Ultrasonic Atomization of Liquids , 1959, IRE Transactions on Ultrasonic Engineering.

[22]  T. K. Mccubbin The Particle Size Distribution in Fog Produced by Ultrasonic Radiation , 1953 .

[23]  A. Loomis XXXVIII. The physical and biological effects of high-frequency sound-waves of great intensity , 1927 .

[24]  J. E. Parsons,et al.  Pulsed cavitational ultrasound therapy for controlled tissue homogenization. , 2006, Ultrasound in medicine & biology.

[25]  J. D. Bassett,et al.  Observations concerning the mechanism of atomisation in an ultrasonic fountain , 1976 .

[26]  L. D. Rozenberg,et al.  Physical principles of ultrasonic technology , 1973 .

[27]  L. Rozenberg Acoustic Atomization of Liquids , 1973 .

[28]  M. N. Topp Ultrasonic atomization-a photographic study of the mechanism of disintegration , 1973 .

[29]  O. K. Eknadiosyants Role of cavitation in the process of liquid atomization in an ultrasonic fountain , 1969 .

[30]  R. J. Lang,et al.  Ultrasonic Atomization of Liquids , 1962 .

[31]  K. Söllner The mechanism of the formation of fogs by ultrasonic waves , 1936 .

[32]  R. W. Wood,et al.  Biological and physical effects of ultrasound , 1927 .

[33]  L. Rayleigh,et al.  The theory of sound , 1894 .

[34]  Michael Faraday,et al.  XVII. On a peculiar class of acoustical figures; and on certain forms assumed by groups of particles upon vibrating elastic surfaces , 1831, Philosophical Transactions of the Royal Society of London.