The acoustic transients associated with optical cavitation in water have been studied using a high-speed interferometric technique . Radial pressure profiles of these spherical transients have been obtained over a range between 2 and 22 mm from the centre of the cavity . Pressure-radius relationships and transient energies have subsequently been determined for the acoustic waves and the volumes of liquid enclosed within them .
. IntroductionThe phenomenon of optical (i .e . laser-induced) cavitation has been studied using a variety of high-speed imaging techniques including Schlieren [1] and streak [2] photography and shadowgraphy [3] . With sufficiently high temporal resolution, all of these methods are capable of visualising acoustic transients formed as a result of cavitation . They do not, however, provide a quantitative measure of the pressures of these transients . They have also tended to rely on conventional photography which is particularly inconvenient in this field of study .In this work, Nd : YAG laser-induced cavitation bubbles and their acoustic transients have been observed in water using a Mach-Zehnder interferometer and a video imaging system . The interferometer was illuminated by a sub-nanosecond light pulse from a nitrogen-pumped dye laser . Interferograms of the cavitation events showed changes in pressure of the liquid as fringe displacements .Previous work in this area has involved the use of transducers and other mechanical methods in measurements of pressure of the acoustic waves . The noncontact high-resolution optical technique used here provides a sensitive measure of transient pressure in cavitation events .
. A simple model of the acoustic waveDuring the early stages of cavitation bubble expansion, the walls of the cavity expand extremely rapidly-faster than the sound speed of the host liquid . The motion of the liquid in the immediate vicinity of the cavity is manifested as a spherical shock wave which travels outwards from the bubble . After a short distance (< 100 pm [4]) the wave slows down to the sound speed and continues as a normal acoustic transient .In this model, the transient was considered to be a step function of liquid pressure . The volume of liquid enclosed within this spherical step was taken to be at a constant pressure, not necessarily equal to the static pressure of the liquid outside . Assuming the width of the step remained a constant, this implied that the peak pressure of the transient was inversely proportional to its radius . Since the volume of 0950-0340/90 $3 . 00