The influence of boiling bubble on the acoustic field and bubble dynamics in histotripsy: A numerical investigation

  • 1State Key Laboratory of Ultrasound in Medicine and Engineering, Chongqing Medical University, Chongqing, 400016, China.
  • 2State Key Laboratory of Ultrasound in Medicine and Engineering, Chongqing Medical University, Chongqing, 400016, China; Chongqing Key Laboratory of Biomedical Engineering, Chongqing Medical University, Chongqing, 400016, China; National Medical Products Administration (NMPA) Key Laboratory for Quality Evaluation of Ultrasonic Surgical Equipment, 507 Gaoxin Ave., Donghu New Technology Development Zone, Wuhan, Hubei, 430075, China; National Engineering Research Center of Ultrasound Medicine, Chongqing, 401120, China. Electronic address: yufeng.zhou@cqmu.edu.cn.

Abstract

Boiling histotripsy (BH) is a non-invasive treatment technique that leverages cavitation effects to disintegrate soft tissue. However, the influence of boiling bubble on the acoustic field and bubble dynamics, which are key mechanisms underlying tissue destruction in BH, is not yet fully understood. This study aims to elucidate the acoustic field distribution and dynamics of a single bubble, demonstrate the generation of intrinsic cavitation bubbles, and predict the associated cavitation damage using a numerical model. The Westervelt equation was employed to simulate the nonlinear propagation of ultrasound pulses in biological tissues, considering varying boiling bubble sizes at the focus and initial acoustic pressures on the transducer surface. Moreover, the Keller-Miksis equation model, combined with the Voigt model, was used to simulate the nonlinear oscillation of bubbles. The presence of a boiling bubble results in significant acoustic reflection at the bubble interface, particularly a notably strong negative pressure. Simulation results show that intrinsic cavitation occurs in a bubble radius of 0.4 mm at an initial acoustic pressure of 2 MPa. Increasing the boiling bubble radius to 1.1 mm leads to the extension of cavitation bubbles toward the second layer of the standing wave field. Additionally, the initial acoustic pressure seems to influence intrinsic cavitation more significantly than the boiling bubble radius. Bubble dynamics, including its maximum bubble radii and expansion duration, is significantly affected by the rarefactional wave. This effect is attributed not only to the peak negative pressure but also to the waveform. In conclusion, the presence of a boiling bubble at the focus substantially modifies the acoustic field distribution, the formation of intrinsic cavitation clouds, and the characteristics of bubble dynamics. The boiling bubble radius and the initial acoustic pressure on the transducer surface are critical factors in modifying cavitation-associated tissue fractionation. Appropriate parameter settings for ultrasonic pulses may enhance the efficacy and reduce the potential complications in BH treatment.

Related Concept Videos

Shock Waves 01:16

2.0K

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...

Sound Waves: Interference 00:53

3.7K

Sound waves can be modeled either as longitudinal waves, wherein the molecules of the medium oscillate around an equilibrium position, or as pressure waves. When two identical waves from the same source superimpose on each other, the combination of two crests or two troughs results in amplitude reinforcement known as constructive interference. If two identical waves, that are initially in phase, become out of phase because of different path lengths, the combination of crests with troughs...

Excess Pressure Inside a Drop and a Bubble 01:13

1.6K

The shape of a small drop of liquid can be considered spherical, neglecting the effect of gravity. This drop can further be considered as two equal hemispherical drops put together due to surface tension. The forces acting on the spherical drop are due to the pressure of the liquid inside the drop, the pressure due to air outside the drop, and the force due to the surface tension acting on the two hemispherical drops.

where γ corresponds to the surface tension. Recalling that the force...

Deriving the Speed of Sound in a Liquid 01:09

486

As with waves on a string, the speed of sound or a mechanical wave in a fluid depends on the fluid's elastic modulus and inertia. The two relevant physical quantities are the bulk modulus and the density of the material. Indeed, it turns out that the relationship between speed and the bulk modulus and density in fluids is the same as that between the speed and the Young's modulus and density in solids.
The speed of sound in fluids can be derived by considering a mechanical wave...

Sound Waves 01:01

9.1K

Sound waves can be thought of as fluctuations in the pressure of a medium through which they propagate. Since the pressure also makes the medium's particles vibrate along its direction of motion, the waves can be modeled as the displacement of the medium's particles from their mean position.
Sound waves are longitudinal in most fluids because fluids cannot sustain any lateral pressure. In solids, however, shear forces help in propagating the disturbance in the lateral direction as well....