An analysis over of character of the isodenses of conical charge explosive products, got by mathematical design, is brought. The features of distribution of the power field are certain depending on direction of initiation of the truncated conical charge. The complex character of intermediate initiator using in a downhole charge as the truncated cone at his location in the ground part of hole is discussed. It is established that the shape of the field of isolines of the density of PD is due primarily to the form of the charge, regardless of the place of its initiation; the prevailing field development occurs relative to the Z axis, that is, along the X axis of the conical charge by the action of its narrow part. This is due to the spread of the products of detonation normal to the sloping surface of the cone. If you associate the total area of the PD density field with the total explosive energy, it is possible to redistribute the flow of energy due primarily to the orientation of the bases and sides of the truncated cone charge, and then to its initiation location. Control of the dynamics and direction of development of the force field is possible by choosing the location of application of the initiating pulse, namely, the location of the initiator on the opposite charge basis for the development of the process in the desired direction of concentrating the energy of the explosion. Due to the specific "pear-shaped" form of the radiated energy field, the explosion of the inverted conical fighter at the stage of initiation of the main (downhole) charge directs the vector of the initial section of the stress wave front towards the upper free surface, ie towards the surface sideways. This area is not subject to the direct action of a system of compressive radial and tensile tangential loads from a charge explosion in a well. changing the direction of development of the force field toward the upper layers of the rock should contribute to better grinding of this part of the array. This method can be implemented using the mechanism of interaction of rock masses, moving towards and additionally destroyed similar to the conditions of short-delay blasting in a schematic diagram, ie, the mechanism of interaction at the level of a slower process - the collision (collision) of the mass directed to the upper side. Simultaneous lower initiation of prolonged charges in adjacent rows gives rise to the front edges inclined to the free surface of the ledge (Fig.). In fact, in this case, the scheme of a wedge or trapezoidal cut is implemented, but oriented instead of the lateral free surface towards the roof of the ledge, which because of its large area is the main source of oversized fractions. consists in the simultaneous simultaneous detonation of three adjacent series of downhole charges treated as one group, followed by the short-term detonation of the adjacent three-row group and the like. The implementation of such a scheme allows to take advantage of its advantages by combining mechanisms of movement of masses in the vertical direction and traditional movement with the coincidence of areas of the array in the horizontal direction. The advantages of using a mixed circuit switching scheme have been proven by industrial testing of the method.
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