Advanced Microwave, Millimeter Wave Technols - Devs, Circs, by A. Mukherjee

By A. Mukherjee

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15. , Shreffler, Willing F. (1954). The limiting conditions for jet formation at high speed. : Mechanics, 1(23), (in Russian). Explosive pulsed plasma antennas for information protection 33 16. , Mali V. (1975). About the influences of viscous of metall to the jet formation process. Fisika gorenia i vzriva (in Russian), Vol. 11, № 1. 17. Karpp. (1976). Criteria for jet formation from impinging shell and plates. J. Appl. , Vol. 47. 18. , Taylor G. (1948). Explosives with lined cavities. J. Of Appl.

The sizes of the CSH material were =7-10, 1525, 80-100 micron. Taking account that the size of the grain on the inner surface of CSH is equal to the size of the surface on the body, fig. 11. From this data, we can see that the size of grain structure on the surface of a high-velocity body greatly influences the electrophysical properties of plasma with CDP. Introducing the particles of metal into the CDP in the plasma track influence it`s electromagnetic properties through thermoelectronic emission from their surface.

Com/doc/6193899/An-Overview-of-the-Shaped-ChargeConcept 27. Dante, J. G. and Golaski, S. K. (1985). Micrograin and Amorphous Shaped Charge Liners. Proceedings of ADPA Bomb and Warhead Section, White Oak, MD, May 1985. 28. Manuel G. Vigil. (2003). Design of Largest Shaped Charge: Generation of Very Large Diameter, Deep Holes in Rock and Concrete Structures. SANDIA REPORT SAND2003-1160, Unlimited Release, Printed April 2003. 29. V. (2002). Physical aspects of shaped charge and fragmentational warheads.

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