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The dynamics, stabilization, and acoustic spectra of a bubble cluster in different liquids are investigated under the condition of ultrasonic cavitation. Experimental data for the dynamics of a spherical ultrasonic cluster near the end face of a rod, capillary, or pressure sensor placed in the antinode of a pressure standing wave at the center of a single-wave spherical piezoelectric concentrator (piezoelectric sphere) are presented. The variation of the cluster size with the parameters of the ultrasonic field and properties of the liquid is studied. It is found that the shape, collapse dynamics, and stability of the cavitation cluster have a significant influence on the acoustocapillary effect. It is shown that the maximal acoustocapillary effect and sonoluminescence are observed when a stable cluster with spherically symmetric collapse dynamics is provided at the end of a capillary in a 50% solution of glycerol. Using a small-size piezotransducer placed at the center of the sphere, the acoustic pressure is measured and acoustic spectra are studied for different voltages across the piezosphere and during the formation of variously shaped cavitation clusters. In the case of fully developed cavitation and a spherical cluster, the acoustic spectra contain subharmonic components, the cavitation noise factor rises to 35%, and the maximum of the noise envelope shifts toward higher frequencies.

The mechanism responsible for the development of autocyclic circular breakdowns in electrolyte as a result of the electric discharge within a hole in a dielectric plate has been experimentally studied. It is demonstrated that the breakdowns are caused by an axisymmetric electrohydrodynamic process involving the formation of a circular bubble breakdown, which acts as a current interrupter in the stage of expansion and as a switch in the stage of collapse, which is followed by the circular breakdown. On the whole, a self-adjusting antiphase process of bubble generation dynamics is developed in the system, whereby each preceding bubble collapses, in the field of pressure due to the subsequent bubble breakdown. This collapse proceeds at an accelerated rate and is accompanied by the fractionation of bubbles.

The early stage of the dynamics of interacting cavitation bubbles in a transmitted spherically focused pulsed wave consisting of compression and rarefaction phases is studied. The cavitation is investigated away from the liquid boundaries for negative pressures up to −42 MPa with a decrease rate of −40 MPa/μs by high-speed microscopic filming (100 million frames per second and a spatial resolution of 5–50μm/pixel) and pressure measurements. It is demonstrated that, according to the kinematics of size variation, the bubbles are separated into two fractions: expanding and collapsing ones. Experimental data provide grounds to assume that the formation of a two-fraction bubble cluster occurs on account of different threshold values of pressure in the rarefaction wave for two characteristic sizes of nuclei, namely, micronuclei (d I < 10μm) and nanonuclei (“bubstons,” d II ∼ 1 nm), which become detectable only when the rarefaction wave amplitude exceeds the critical one. Pulsed compression of small bubbles in the process of transformation of a rarefaction wave into a compression wave occurs under the effect of a cluster’s internal pressure up to 20 MPa and proceeds with the conservation of the spherical shape of the second-fraction bubbles. It is demonstrated that the velocity of the center of mass of a bubble reaches its peak value close to the moment of bubble collapse. The translational and radial dynamics of a bubble are studied in a numerical experiment using the Rayleigh-Plesset equation and taking into account the viscous force and the pressure gradient. The results of measuring the translational shift may be useful for estimating the minimum bubble radius by comparing the numerical results with the experiment.

To elucidate mechanisms of cavitation action on a surface with microcapillary discontinuity and refine the model of the sonocapillary effect, the force acting on a cylinder is correlated with the height of a liquid in the capillary under cavitation, both quantities being measured at the same point of the ultrasonic field. It is found that the force acting on the cylinder is directed toward a cavitation cluster stabilized at the end face of the cylinder. This force can be enhanced with another cylinder placed on the side of the cluster coaxially with the first one. The dynamics of the cavitation cluster depending on the cylinder spacing is investigated in the case when one of the cylinders is on a pendulum suspension. The conditions for self-sustained oscillations of the pendulum are found. The dependence of the attracting force between the cylinders on the ultrasonic frequency and cylinder spacing is derived. The end-face-averaged pressure exerted on a cylinder of diameter 1.2 mm may reach 0.16 kPa, and the intracapillary pressure attains 0.89 kPa. Thus, the sonocapillary effect may be explained, at least partially, by a counterpressure arising from cluster-capillary interaction. This effect can be used in designing cavitation sensors and ultrasonic sources.

The determination of the phase of the bubble oscillation at the instant of light emission, which is a key issue for understanding the origin of cavitation luminescence of liquids, is discussed. The observation of luminescence in the course of the nucleation and growth of a bubble up to its collapse is performed in a bipolar wave consisting of a compression phase followed by a rarefaction phase in the regime of a two-fraction bubble cluster formation. The space-time distributions of the luminescence intensity and pressure and the dynamics of the cluster in water and a glycerin solution are investigated at the early stage of cavitation. A correlation between the maximal density of light flashes and the positive pressure pulses in the field of superposition of the initial and secondary cavitation compression waves is revealed. It is shown that the spherical focusing of acoustic pulses both away from the boundaries of the liquid and near its free surface makes it possible to compare the luminescence intensities for different rates of the pressure decrease.

Nonlinear processes accompanying the focusing of a microsecond acoustic pulse produced by an electromagnetic source shaped as a spherical segment are investigated. The processes are considered to be far from the boundaries of a liquid, in the absence of cavitation. Detailed measurements of the pressure field by a fiber-optic sensor and high-speed photography of the shock front are performed. The pressure field is found to be determined by the nonlinear effects that occur in the course of the propagation of the initial converging compression wave and an edge rarefaction wave. The peak pressure amplitudes at the focus are 75 and −42 MPa for the compression and rarefaction waves, respectively, at the maximum voltage of the pulse generator in use. The measured length of the compression wave front is equal to the response time of the sensor (8 ns). The pressure amplitude is shown to be limited by the irregularity of the propagation of a shock wave in the form of Mach’s disk. At the focus, the pressure gradient across the radiator axis reaches 0.5 atm/μm, while the diameter of the focal spot is 2.5±0.2 mm. The focus of the edge rarefaction wave formed due to diffraction is located closer to the radiator than the focus of the compression wave, which may facilitate the study of the biological effect of cavitation independently of the shear motion of the medium.

Slow variation (for 10–40 min) of the electrical conductivity of a water cell in weak permanent magnetic fields was studied. Relaxation characteristics and the dependence of the resistivity on a magnetic field ranging between 0.02 and 0.11 G were obtained. It was found that the cell response lags behind magnetic field switching-on and switching-off.

Results are presented of experimental investigations of the dynamics of the electrical conductivity of an electrolyte when one of the electrodes is exposed to a weak shock pulse. It is shown that the electrical conductivity in the cell increases as a result of damage to the electric double layer.