Detonation in stratified two-phase systems “gaseous oxidizer – liquid fuel film”: three-dimensional simulation
- Authors: Ivanov V.S.1,2, Frolov S.M.1,2, Semenov I.V.2
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Affiliations:
- N. N. Semenov Federal Research Center for Chemical Physics of the Russian Academy of Sciences
- Scientific Research Institute for System Analysis of the Russian Academy of Sciences
- Issue: Vol 17, No 4 (2024)
- Pages: 65-81
- Section: Articles
- URL: https://journals.rcsi.science/2305-9117/article/view/284445
- DOI: https://doi.org/10.30826/CE24170407
- EDN: https://elibrary.ru/FRQEKY
- ID: 284445
Cite item
Abstract
The article presents the results of multidimensional numerical calculations of direct detonation initiation and deflagration-to-detonation transition (DDT) in horizontal flat channels of different height filled with gaseous oxygen under normal conditions and with films of -heptane and -decane applied to the lower wall. The determining role of liquid fuel volatility in the mechanism of film detonation propagation is shown. The mechanism of detonation propagation in the system with an -heptane film is self-ignition of fuel vapors in the gas phase and in the system with an -decane film, it is the mechanical destruction of the film, evaporation of the resulting microdroplets, and self-ignition of fuel vapors in the gas phase. It is shown that during DDT in channels of different height with an -heptane film, preflame secondary explosions leading to DDT occur in a shock-compressed mixture of oxygen with preevaporated fuel near the leading shock wave (SW) but at a large distance from the film — in areas with elevated temperature and increased gas residence time. The SW velocity at the time of DDT is 800–900 m/s and the resulting detonation wave (DW) propagates at a speed exceeding 1300 m/s. At low ignition energies, there may be two limiting values of the channel height — minimum and maximum — at which DDT is still possible. The minimum channel height is determined by momentum and energy losses on the walls and the maximum is determined by the presence of an additional mechanism for evening the pressure in the flame.
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About the authors
Vladislav S. Ivanov
N. N. Semenov Federal Research Center for Chemical Physics of the Russian Academy of Sciences; Scientific Research Institute for System Analysis of the Russian Academy of Sciences
Author for correspondence.
Email: ivanov.vls@gmail.com
(b. 1986) — Doctor of Science in physics and mathematics, leading research scientist, N. N. Semenov Federal Research Center for Chemical Physics of the Russian Academy of Sciences; research scientist, Federal State Institution “Scientific Research Institute for System Analysis of the Russian Academy of Sciences”
Russian Federation, 4 Kosygin Str., Moscow 119991; 36-1 Nakhimovskii Prosp., Moscow 117218Sergey M. Frolov
N. N. Semenov Federal Research Center for Chemical Physics of the Russian Academy of Sciences; Scientific Research Institute for System Analysis of the Russian Academy of Sciences
Email: smfrol@chph.ras.ru
(b. 1959) — Doctor of Science in physics and mathematics, head of department, head of laboratory, N. N. Semenov Federal Research Center for Chemical Physics of the Russian Academy of Sciences; professor, National Research Nuclear University MEPhI (Moscow Engineering Physics Institute); leading research scientist, Federal State Institution “Scientific Research Institute for System Analysis of the Russian Academy of Sciences”
Russian Federation, 4 Kosygin Str., Moscow 119991; 36-1 Nakhimovskii Prosp., Moscow 117218Ilya V. Semenov
Scientific Research Institute for System Analysis of the Russian Academy of Sciences
Email: ilyasemv@yandex.ru
(b. 1973) — Candidate of Science in physics and mathematics, head of department
Russian Federation, 36-1 Nakhimovskii Prosp., Moscow 117218References
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