By E. Krause
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Additional resources for Eighth International Conference on Numerical Methods in Fluid Dynamics: Proceedings of the Conference, Rheinisch-Westfälische Technische Hochschule Aachen, Germany, June 28 – July 2, 1982
Blast of charges of condensed explosive Two stages may be distinguished in this process. The first stage includes the initiation and the development of detonation in condensed explosive. The motion of gaseous products of blast and the shock wave propagation into an ambient media proceed at the second stage. A series of works are devoted to the numerical simulation of the first stage onlyo Among them the monograph by ~ader ( 1979 ), which involves also two-dimensional cases, is the most fundamental.
M. ( 1978 ) Arch. Mech. Stosow. 30, 553-571. R. ( 1979 ) AIAA Journal 17, 601-605. S. ( 1977a ) Uch. Zap. Tsentr. Aero-Gidrodinam. Inst. 3, 32-38. S. ( 1977b ) Zh. Vychisl. Mat. i Mat. Fiz. 17, 1325-1329. N. ( 1970 ) Phys. Fluids 13, 2665-2675. I. ( 1979 ) Kvant. Electronika 6, 379-381. I. ( 1980 ) Dokl. AN BSSR 24, 702-705. I. ( 1977 ) Zh. Vychisl. Mat. i Mat. Fiz. 17, 1602-1607. E. ( 1975 ) J. Comput. Phys. 17, 132-159. V. ( 1980 ) Dokl. AN SSSR 252, 318-322. A. ( 1976 ) Lect. Notes Phys. 59, 384-390.
All the characteristics of the undisturbed air along the rays are taken in accordance with their actual values in the atmosphere. This model does not allow for interactions of gas motions in each sector and energy redistribution between them. Therefore, the model appears to be reliable only to a certain extent. In the framework of this approximation, Lutzky and Lehto ( 1968 ) computed the propagation of descending shock waves caused by spherical explosions in exponential atmospheres with various non-homogeneity scales.
Eighth International Conference on Numerical Methods in Fluid Dynamics: Proceedings of the Conference, Rheinisch-Westfälische Technische Hochschule Aachen, Germany, June 28 – July 2, 1982 by E. Krause