transferable over a long distance, but this requires substantial energy and also imposes limits on the particle size, moisture content of the material, and uniformity of physical properties. In this work we have studied a new pulse gas-dynamic technique of friable material transportation, which proposes to eliminate the above-mentioned drawbacks. The essential feature of the technique is cyclic ejections of compressed gas from gas sources lying deep under a friable material bed. The sources are snapped into action in the "travelling wave" mode, in which an ejection cone as well as a camouflet (underground explosion cavity) may be the external manifestation of each pulse [2]. In physical nature, this process is similar to the phenomenon of directed excavating explosion well known in explosion engineering, but in this case the material moves within the confined space of the transport trough. Studies were made earlier to determine the local transportation index for both cone and camouflet formation [2]. The studies were aimed at deciphering the most effective range of parameters, in which the material transportation process, at a fLxed consumption of the energy of the gas, is optimum. It was shown that the most acceptable is that range of parameters on combination of which is formed, in the case of singular actuation of the gas source, a limiting camouflet or a cone with a small ejection activity index fi = 0.4-0.7, fi being the ratio of the cone radius to the source depth. However, previous studies examined actuation of only a pair of sources where symmetric ejection of the first source in a bed of an unagitated friable material is preparatory and the next (directed) one is operating. In real transporting situations, on the other hand, the operating ejection of the preceding source is preparatory, i.e., the physical pattern of development of the phenomenon is different. This necessitates an assessment of the efficiency of the pulse pneumatic transporter and precise determination of the optimal combination of the starting paraxneters. The following should be distinguished as the key factors governing the rate of development of the phenomenon. The energy E of the gas in a pulse, whose scale can be depicted via the full ejection energy, with due regard for the degree of gas expansion [3], is: