Study of the effect of high pressures on the deformation properties of rocks has an important bearing on faster development of mineral deposits. The inadequacy of analytical methods of calculation, and of methods of simulating deformation processes for solving practical problems, is due to insufficient experimental research. Experimental data on the deformation properties of rocks are scanty and do not enable us to develop a schematic functional model of the medium being deformed [1][2][3]. In particular, the litmrature does not give correlating data on the effect of hydrostatic stress on the deformation and strength properties of the rocks of a sedimentary succession to which mined minerals belong. This paper gives data on the deformation properties of Mesozoic sandstones and siltstones under high pressures. Such investigations are important for developing effective schemes of rock breaking by drilling.The mechanical methods of breaking used in mining are based chiefly on driving tools into the rock. This is the basic process in percussive, chilled-shot, and roller-bit drilling. In roller-bit drilling, rotation of the rollers against the face is accompanied by indentation of the teeth into the rock; the axial load is transmitted via small contact areas.The partlcular characteristic ofexperimentalwork on the strength and deformation properties of in-situ rocks is the buLk characlmr of the stalm of stress. In research on drilling cores with the objective of simulating face conditions, a hydrostatic stress is created, and a cylindrical punch with a flat base is forced into a specimen of the rock. The fracture mechanism of the latter is determined by the stress field beneath the punch and by the properties of the rock itself. With the use of the sophisticated theory of elasticity for calculating the stress field, the rock is considered to a first approximation as an elastic uniform half-space.When the punch is driven into the rock, under conditions of volumetric stress a limiting sl~ess arises at a certain depthTills stressed state Is axially symmetric, and the distribution of radial, circumferential, and axial normal stresses o r, o0, and Oz, which are the principal stresses, may be expressed as follows [4]: ~r = ~o = 1/" a2 + z2 ~/a~ + z2 ; Z3