The study of the vicinity of the explosion, and in particular the development of the cavity, is the key m the problem of energy distribution due m detonation of a charge in a solid.Theoretical attacks on the problem of the development of a cavity and the changes in the gas Pressure inside it involve grave mathematical difficulties due m the compressibility of the medium and the consequent formation of a shock wave.This served as a basis for special experlrnenml invesffgatlons which led m an analytical solution which was explained in princlple in [1]. The aims of this work were m develop a method of experlmenml Investigaffon, further study of the physical essence of the phenomena occurring near r_he explosion, and in particular determination of the changes in the position of the inmrior walls of the cavit 7 and their maximum radial deviation from ~elr initial position.Demnatlon of spherical charges and the consequent formation and development of a cavity in media possessing mechanical strength were first studied in/he USSR by the x-ray method [2,3].This merlin d of recording rapid processes, especially those near an explosive charge, is in our o pinion the most promising one, and the experimental data accumulamd by ntis means are very useful Method of Investiyarlon. The kinemaffc paramemrs of the development of a cavity around a charge chamber in dynamic condilJons were registered by means of x-rays. The pulsed x-ray apparatus consisted of a voltage pulse general)to x-ray tubes, a vacuum system for creating and maintaining the high vacuum, delay lines m trigger the x-ray robes, fLd.ng circuits, and other auxiliary units.The voltage pulse generators, charged via a rectifier, gave 800 kV pulses which were fed m the electrodes of the x-ray robes. During the initial stage of vacuum breakdown of the interelectmde gap a very short-lived (0.15 0.20 sec) x-ray pulse is emitted. Owing to the delay lines in the generator discharge circuits, the voltage pulses ~o /he x-ray tubes are triggered in sequence at microsecond intervals. The duration of emission by each tube is at most 2 -10 -7 sec. Triggering of each tube was delayed 2-7 ~sec behind the preceding one. A circuit for measuring the time intervals between the triggering of each tube enabled us/D make oscillograph records of the marks corresponding to each x-ray pulse.The specimen was placed in the center of an explosion chamber, round which the sharp-focus x-ray tubes were arranged around a 90-degree arc (Fig. 1).The photographs were exposed on x-ray film in cassettes in the explosion chamber exactly opposite the specimen and x-ray tubes.Interpretation of the x-ray pho~ographs reduced m measuring the radius of the cavity on the prints and measurement of the time intervals as the radius expanded. We ~ook account of the coefficient of geomelzical magnification of the images, which was 1.18 in our experimental conditions. G. V. Plekhanov Mining Institum, Leningrad.