Influence of the thickness and absorption coefficient of a copper oxide film on the ignition delay of PENT by a laser pulse

Bibliographische Detailangaben
Parent link:Combustion, Explosion, and Shock Waves.— , 1965-
Vol. 52, iss. 1.— 2016.— [P. 91-95]
Körperschaften: Национальный исследовательский Томский политехнический университет Юргинский технологический институт (филиал) Кафедра естественного научного образования, Национальный исследовательский Томский политехнический университет Энергетический институт Лаборатория моделирования процессов тепломассопереноса
Weitere Verfasser: Khaneft A. V. Aleksandr Villivich, Dolgachev V. A. Vadim Aleksandrovich, Zverev A. S. Anton Sergeevich, Mitrofanov A. Yu. Anatoliy Yuryevich
Zusammenfassung:Title screen
Numerical modeling of PETN ignition by a copper oxide film absorbing laser radiation has been performed. The calculation results showed the presence of a minimum in the curve of the dynamic delay of PETN ignition by a rectangular laser pulse versus thickness of the absorbing film. This effect is due to the fact that when the film thickness is commensurate with the reciprocal of the absorption coefficient, the amount of heat generated in the thin film due to the multiple reflection of the light flux is proportional to its thickness. Therefore, the smaller the film thickness, the more time is required to heat it to the ignition temperature of PETN. In the case of a thick film, additional energy and time are required to heat its cold part to the ignition temperature of PETN.
Режим доступа: по договору с организацией-держателем ресурса
Sprache:Englisch
Veröffentlicht: 2016
Schlagworte:
Online-Zugang:http://dx.doi.org/10.1134/S0010508216010123
Format: Elektronisch Buchkapitel
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=648275
Beschreibung
Zusammenfassung:Title screen
Numerical modeling of PETN ignition by a copper oxide film absorbing laser radiation has been performed. The calculation results showed the presence of a minimum in the curve of the dynamic delay of PETN ignition by a rectangular laser pulse versus thickness of the absorbing film. This effect is due to the fact that when the film thickness is commensurate with the reciprocal of the absorption coefficient, the amount of heat generated in the thin film due to the multiple reflection of the light flux is proportional to its thickness. Therefore, the smaller the film thickness, the more time is required to heat it to the ignition temperature of PETN. In the case of a thick film, additional energy and time are required to heat its cold part to the ignition temperature of PETN.
Режим доступа: по договору с организацией-держателем ресурса
DOI:10.1134/S0010508216010123