The aim of this 1972 guide is to take the wealth of knowledge accrued through the military over a interval of years almost about hardening weapon structures opposed to RF power and to make this knowledge to be had to the clothier. a lot of the knowledge during this guide is in chart or desk shape for speedy retrieval. even though this guide used to be ready for the fashion designer of weapon platforms it may even be of profit to these engaged in designing attempt courses for making a choice on the hardening of weapon platforms.
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Extra resources for Engineering Design Handbook - Hardening Weapon Systems against RF Energy:
4-3. The charge developed by this operation may be sufficient to burn out the junction of the transistor. Any weapon system circuit that uses solid state devicesshould be shielded completely so that no charge can be induced into that circuit. There is no MIL-STD for static electricity tests on EED's; however, MIL-I-23659, Initiators. Electric. Design and Evaluation oj(Ref. 4. 4. 3, twelve initiators shall be subjected to the following tests. A 500 micromicrofarad ±5% capacitor charged to 25,000 ±500 volts and a 5000 ohm ±5% resistor shall be connected in series between pairs of pins or leads in all combinations and between the shorted pins or leads (all pins or leads shorted to each other external to the initiator) and the case.
2-12 and 2-14. More is said concerning the discharge process in par. 5. Repeats of these phenomena are common. The stepped leader is generally replaced by a "dart" leader that re-establishes the path from earth-to-cloud for all strokes other than the first in a series. 2 CURRENT AND CHARGE The magnitude of current, initial charge, and charge height varies widely from discharge to discharge. This factor alone probably accounts for much confusion in the theoretical and experimental treatment of lightning data.
For weapon system shields, and almost all other practical applications of shielding for that matter, the classical shielding effectiveness does not correctly relate the power densities. Furthermore, the results so obtained may be greater than, equal to, or less than the actual values. In general, the results 4-1 AMCP 706·235 normally predict a power density inside the shielded volume which is much lower than the actual value. Since the actual shielding effectiveness of a shield depends heavily upon the geometry of the shield and, more important perhaps, on what the shield contains and its position, it would seem important to determine this dependence.