1972
DOI: 10.1016/0376-0421(72)90017-6
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Appraisal of UTIAS implosion-driven hypervelocity launchers and shock tubes

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Cited by 17 publications
(2 citation statements)
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“…For example, while a hypervelocity launcher in which a spherically imploding wave is focused onto a projectile can, in theory, generate projectile velocities in excess of 10 km/s, in practice, the projectile is unable to survive the intense loading at the focus point of the implosion. 2 Alternatively, if the implosion process is distributed continuously along the launch tube, the projectile loading can be maintained at a nearly constant moderate level for the entire launch cycle (note that "moderate" may still mean accelerations as great as 10 8 m/s 2 ).…”
Section: Introductionmentioning
confidence: 99%
“…For example, while a hypervelocity launcher in which a spherically imploding wave is focused onto a projectile can, in theory, generate projectile velocities in excess of 10 km/s, in practice, the projectile is unable to survive the intense loading at the focus point of the implosion. 2 Alternatively, if the implosion process is distributed continuously along the launch tube, the projectile loading can be maintained at a nearly constant moderate level for the entire launch cycle (note that "moderate" may still mean accelerations as great as 10 8 m/s 2 ).…”
Section: Introductionmentioning
confidence: 99%
“…However, it is not clear whether or not converging shock waves are stable. Glass (1972) constructed a hemispherical implosion chamber and Saito & Glass (1982) succeeded in imploding a hemispherical shock wave at its centre. Extremely high pressures and temperatures were generated at the focal zone in proportion to the amount of energy released, but the stability of imploding shock waves was not discussed.…”
Section: Introductionmentioning
confidence: 99%