2018
DOI: 10.1109/tmtt.2017.2772801
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On the Differential Input Impedance of an Electro-Explosive Device

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Cited by 8 publications
(8 citation statements)
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“…In such cases, side-walls of the pipe were thrown first; the average fragment velocity was ∼1000 km/s ∗ 1 . In deflagrations, the end cap was first thrown; fragment velocities were only ∼240 km/s ∗ ” [ 938 ].…”
Section: Other (Safety Definitions Etc)mentioning
confidence: 99%
“…In such cases, side-walls of the pipe were thrown first; the average fragment velocity was ∼1000 km/s ∗ 1 . In deflagrations, the end cap was first thrown; fragment velocities were only ∼240 km/s ∗ ” [ 938 ].…”
Section: Other (Safety Definitions Etc)mentioning
confidence: 99%
“…These combinations represent different objects. Short and long wires are represented with elements with a radius of 0.05 mm and lengths of 5 and 20 cm, respectively, a pipe is represented with an element of 20‐cm length and 2.5‐mm of radius, and an electric igniter is represented with an element of 5‐cm length and 2.5‐mm radius (Pantoja et al, ). Table shows that the variation in the soils produces a variation higher than 12% in the first resonance frequency.…”
Section: Electromagnetic Coupling To a Buried Wirementioning
confidence: 99%
“…9 Michael R. Lambrecht and John J. Pantoja regard the EEDs pin as a non-uniform transmission line to obtain its input impedance, 10 and the coupling current of the pin wire is determined by the matrix equation of the coupling telegraph. 11 Many researchers represented by two-pin wire types all kinds of EEDs have conducted a series of theories and experiment on electromagnetic environment effects, which have made some progress and achievements. However, these efforts have not considered the antenna model structure formed by EEDs caused by the internal structure of the equipment.…”
Section: Introductionmentioning
confidence: 99%
“…In addition, in the electromagnetic protection of two‐pin bridge wire, electric explosives, the coupling induced current on the pins will increase significantly at the resonant frequency point, which can be calculated by analytical formulas 9 . Michael R. Lambrecht and John J. Pantoja regard the EEDs pin as a non‐uniform transmission line to obtain its input impedance, 10 and the coupling current of the pin wire is determined by the matrix equation of the coupling telegraph 11 …”
Section: Introductionmentioning
confidence: 99%