Download EMP: Environment and System Hardness Design by Dr. Rabindra N. Ghose PDF

By Dr. Rabindra N. Ghose

Nuclear EMP is surveyed with its impression on digital structures and vulnerability and process hardness verification. assets of EMP and the ensuing surroundings are reviewed together with the mechanism of the EMP box, deposition zone and ensuing EM degrees for high-altitude, flooring and near-ground and underground bursts. inner EMP and system-generated EMP are mentioned. lined intimately are the access modes of EMP strength into platforms.

Coupling types comprise cables and transmission traces performing as antennas in various configurations and during shields and enclosures, apertures, slots and slits, and during application structures. EMP susceptibilities in digital structures comprise circuit vulnerability, latchup, everlasting harm and burnout. Prediction & research through math types of move services of assets, media, coupling & sufferers are provided. The approach can be analyzed through vulnerability prediction and the technique is mentioned intimately together with zoning & coupling analysis.

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Extra resources for EMP: Environment and System Hardness Design

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5 x 10-5 y r the field at the center of the cylinder being zero. 17) volts The magnetic field produced for such a case is given by: H = -2 x 10-8 . 19) Cylindrical Enclosure~;<: Wall y . 19 - Illustration of the Cavity-mode of IEMP Generation. 20 - Internal EMP Field Components. 24 Sec. 2. 19. 19, the E-field remains the sa_me and the magnetic field has the same magnitude as before but has a different direction, as shown in Figure 2. 21. 2) To obtain an estimate of the IEMP characteristics to be expected realistically, one may assume a value of y = 10 8 (Routgens/sec).

A \survey and organization of this information are attempted in the following chapters. 5 1. oion, c. E. Trans. AP-26, 1978. L6e P~odueed by Nuele~ 2. Brown, G. , Ghose, R. , Green, J. , Putzer, E. , and Wouters, L. L6e En~gy Stud-le~, American Nucleonics Corporation, Glendale, California, February 1967. 3. Vance, E. I. International, California, Fourth Symposium and Technical Exhibition on Electromagnetic Compatibility, Zurich, March 1981. 8 CHAPTER 2 Sources of EMP and EMP Environment Prompt gamma rays which follow the nuclear detonation are the principal source of EMP.

7) q being the electric charge of an electron, since the electric current is just the charge in motion. One needs to determine the conductivity of~the medium in addition to the driving current density 1a to evaluate E and B components of the EMP field. This conductivity is due to the interactions of gamma and other nuclear radiations with the air and materials surrounding the location of burst and can be determined by summing the contributions from various charged species. n. 8) qi is the charge of the ith species µi is the mobility of the ith species ni is the number density of the ith species.

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