2024-03-29T00:12:47Z
https://tsukuba.repo.nii.ac.jp/oai
oai:tsukuba.repo.nii.ac.jp:00028310
2022-04-27T08:56:19Z
2871:2874:1464
3:62:5598:1651
Front shock behavior of stable curved detonation waves in rectangular-cross-section curved channels
笠原, 次郎
Nakayama, Hisahiro
Kasahara, Jiro
Matsuo, Akiko
Funaki, Ikkoh
© 2012 The Combustion Institute.
NOTICE: this is the author’s version of a work that was accepted for publication in Proceedings of the Combustion Institute. Changes resulting from the publishing process, such as peer review, editing, corrections, structural formatting, and other quality control mechanisms may not be reflected in this document. Changes may have been made to this work since it was submitted for publication. A definitive version was subsequently published in Proceedings of the Combustion Institute, 34, 2, 2013, DOI:10.1016/j.proci.2012.06.012.
The propagation of curved detonation waves of gaseous explosives stabilized in rectangular-cross-section curved channels is investigated. Three types of stoichiometric test gases, C2H4 + 3O2, 2H2 + O2, and 2C2H2 + 5O2 + 7Ar, are evaluated. The ratio of the inner radius of the curved channel (ri) to the normal detonation cell width (λ) is an important factor in stabilizing curved detonation waves. The lower boundary of stabilization is around ri/λ = 23, regardless of the test gas. The stabilized curved detonation waves eventually attain a specific curved shape as they propagate through the curved channels. The specific curved shapes of stabilized curved detonation waves are approximately formulated, and the normal detonation velocity (Dn)−curvature (κ) relations are evaluated. The Dn nondimensionalized by the Chapman–Jouguet (CJ) detonation velocity (DCJ) is a function of the κ nondimensionalized by λ. The Dn/DCJ−λκ relation does not depend on the type of test gas. The propagation behavior of the stabilized curved detonation waves is controlled by the Dn/DCJ−λκ relation. Due to this propagation characteristic, the fully-developed, stabilized curved detonation waves propagate through the curved channels while maintaining a specific curved shape with a constant angular velocity. Self-similarity is seen in the front shock shapes of the stabilized curved detonation waves with the same ri/λ, regardless of the curved channel and test gas.
Elsevier Inc.
2013
eng
journal article
http://hdl.handle.net/2241/118452
https://tsukuba.repo.nii.ac.jp/records/28310
10.1016/j.proci.2012.06.012
1540-7489
AA11552208
Proceedings of the Combustion Institute
34
2
1939
1947
https://tsukuba.repo.nii.ac.jp/record/28310/files/PROC-CI_34-2-1939.pdf
application/pdf
1.4 MB
2013-12-25