Original Contribution
Investigation into the Mechanisms of Tissue Atomization by High-Intensity Focused Ultrasound

https://doi.org/10.1016/j.ultrasmedbio.2014.12.022Get rights and content

Abstract

Ultrasonic atomization, or the emission of a fog of droplets, was recently proposed to explain tissue fractionation in boiling histotripsy. However, even though liquid atomization has been studied extensively, the mechanisms underlying tissue atomization remain unclear. In the work described here, high-speed photography and overpressure were used to evaluate the role of bubbles in tissue atomization. As static pressure increased, the degree of fractionation decreased, and the ex vivo tissue became thermally denatured. The effect of surface wetness on atomization was also evaluated in vivo and in tissue-mimicking gels, where surface wetness was found to enhance atomization by forming surface instabilities that augment cavitation. In addition, experimental results indicated that wetting collagenous tissues, such as the liver capsule, allowed atomization to breach such barriers. These results highlight the importance of bubbles and surface instabilities in atomization and could be used to enhance boiling histotripsy for transition to clinical use.

Introduction

Ultrasonic atomization is a process that occurs when an acoustic wave in liquid is directed toward an air interface (a pressure-release interface); the process is not simple when the incident wave is a plane wave, and it becomes even more complex when the incident wave is a narrow, focused beam. Although liquid atomization has been studied extensively since the discovery of atomization in 1927, there remains some doubt as to the exact mechanism (Rozenberg, 1973, Simon et al., 2012). The most accepted hypothesis of liquid atomization, called the cavitation-wave hypothesis, states that atomization arises from a combination of cavitation bubble oscillations and capillary wave instabilities (Boguslavskii and Eknadiosyants, 1969, Rozenberg, 1973). Recently, it was reported that tissues could also be atomized and that such atomization occurs in the form of fractionation and expulsion of tissue from the surface (Simon et al. 2012). Yet questions remain as to the mechanism underlying tissue atomization, particularly the roles of bubbles and tissue properties in the fractionation and atomization of tissue. The goal of the work described in this article was to test experimentally the role of cavitation in the fragmentation and atomization of ex vivo tissue by suppressing bubble activity with overpressure. The effects of tissue properties were also investigated, in particular how the wetness of tissue and its surface affect the inception and success of atomization and surface erosion in vivo and in tissue-mimicking gels.

Tissue atomization was first explored to explain the mechanism of bulk tissue fractionation in a relatively new high-intensity focused ultrasound (HIFU) approach named boiling histotripsy (Simon et al. 2012). In boiling histotripsy, non-linear propagation effects result in the formation of high-amplitude shocks in the ultrasound pressure waveforms and shock-wave heating causes the formation of a millimeter-diameter boiling bubble at the transducer focus in milliseconds (Canney et al. 2010). Interaction of the incident ultrasound wave with the bubble results in the fractionation of tissue into its submicron components (Khokhlova et al., 2011, Wang et al., 2013). With thorough experimentation, it was found that a fountain could form and atomization could occur within a millimeter void that mimicked the HIFU-induced boiling bubble in tissue; that the end result of atomization was erosion of the flat tissue surface adjacent to the air; and that the atomized tissue expelled from the flat tissue surface was partially fractionated, though not to the extent observed in bulk boiling histotripsy (Simon et al. 2012). By better understanding the mechanism of tissue atomization, the safety and efficacy of tissue fractionation by boiling histotripsy can be enhanced in its further development and transition into a clinical therapy.

Several observations were made during these preliminary studies, leading to questions regarding the mechanism of tissue atomization. For example, in the initial studies it was observed that the time the ex vivo tissue spent submerged in phosphate-buffered saline (PBS) affected the rate of tissue atomization and erosion (Simon et al. 2012), leading to the idea that tissue wetness influences atomization. Submersion in PBS is known to cause tissue swelling because of the changes in cellular metabolism and differences in salt and sugar concentrations between the tissue and solution, which affect not only tissue wetness, but also the mechanical stiffness of the tissue (Boutilier, 2001, Kaboyashi et al., 1991, Southard, 2004). In addition, PBS could also influence atomization by forming a thin liquid layer on the tissue surface that could ease the formation of capillary waves or other surface instabilities. Another observation made during preliminary studies was that highly collagenous tissues such as the liver capsule are more difficult to atomize. This relates back to both boiling and cavitation-cloud histotripsy therapies, where it has been noted that highly elastic tissues, such as blood vessels, remained intact while the surrounding tissue was completely fractionated (Khokhlova et al., 2014, Vlaisavljevich et al., 2014). Investigation into the influence of tissue viscoelasticity and wetness on its atomization could help in determining the tissue types that can be successfully atomized, as well as enhancing our understanding of the fundamentals of the mechanisms of tissue atomization by ultrasound.

In liquids, the cavitation-wave hypothesis most accurately describes what is observed in atomization; however, in tissues there is much debate as to whether atomization can be similarly described. In this article, the hypothesis that bubbles are necessary for tissue atomization was tested. The effect of bubbles was controlled by applying excess static pressure to the tissue samples studied. Overpressure has been used in other ultrasonic applications such as HIFU thermal ablation and shock wave lithotripsy to assess the role of bubbles (Bailey et al., 2001, Bronskaya et al., 1968, Hill, 1971, Khokhlova et al., 2006, Sapozhnikov et al., 2002). In this work, the role of cavitation in tissue atomization was established using a custom-designed overpressure chamber and a high-speed camera. In addition, the effect of tissue wetness on atomization was evaluated, considering the relative effects of bulk and surface wetness on the erosion volume in ex vivo tissues and tissue-mimicking gels. High-speed photography was also used to analyze atomization in vivo, and techniques to breach the collagenous porcine liver capsule were explored. Finally, the hypothesis of tissue fragment recirculation was investigated to explain the histologic differences between bulk boiling histotripsy and atomization. As atomization has been found to explain the mechanism of tissue fractionation in boiling histotripsy, the ultrasound frequency, pulse length and pulse repetition frequency were chosen based on those used in most of the previously reported boiling histotripsy studies (Khokhlova et al., 2011, Khokhlova et al., 2014, Wang et al., 2013). Although the figures and supplementary videos included in this article illustrate single instances of atomization, they represent what was observed upon repeated experimentation.

Section snippets

Effect of overpressure on atomization

The custom-built overpressure chamber with a 2.127-MHz aluminum-lensed HIFU transducer is illustrated in Figure 1. The transducer consisted of a flat, 40-mm-diameter, piezoceramic source and an aluminum lens with a center thickness of 10.8 mm and a focal length of 40 mm. The static pressure in the chamber was controlled using a compressed air cylinder with a regulator (ProStar 4092, Praxair, Seattle, WA, USA). To create a pressure-release interface at the focal plane with adequate acoustic

Effect of overpressure on atomization

As illustrated in Figure 3, at atmospheric pressure and the in situ intensity of 22 kW/cm2 (p+ = 67.4 MPa, p− = −16.4 MPa), atomization of bovine liver with the aluminum-lensed transducer proceeds similarly to what was observed previously (Simon et al. 2012); droplets are released from a mound in bovine liver at velocities of approximately 5–7 m/s, ranging in diameter from less than 1 pixel (20 μm) up to 180 μm. However, when the static pressure is increased even to 1.4 MPa, atomization of

Discussion

Evidence from these studies supports both surface instabilities and bubble activity as contributors to tissue atomization. In the first study, overpressure was used to illustrate that bubbles are important to tissue fractionation by atomization; as the static pressure of the system increased, the degree of tissue fractionation decreased. It was difficult to discern whether these bubbles arose from acoustic cavitation or heat deposition and boiling. That there was no apparent change in the

Acknowledgments

The authors thank our collaborators at the Center for Industrial and Medical Ultrasound. In particular, we thank Dr. Ziyue Liu at Indiana University for performing the statistical analysis on the large amounts of data collected in the bulk tissue wetness studies. We also thank Ameen Tabatabi for his help in the bulk wetness studies, Frank (Rusty) Starr III for his help in the in vivo studies, Dr. Wayne Kreider for his helpful discussions in bubble dynamics and Brian MacConaghy for designing,

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