“…In the case of a brittle transverse crack moving at a constant rate, the length of this segment is proportional to d; therefore, from (2) substituting L = nd, where n = const and d = const, we obtain σ = const. (1) and maximum rates of wall displacement (2) for shells of various scales versus the relative mass of the explosive charge: points , , , and refer to samples of type I and points •, , •, and to samples of type II; light symbols indicate that the samples that did not fail and dark symbols indicate that the samples that failed (through cracks formed) [34].…”