Experimental study of the perturbation of the cavity on the deflagration to detonation transition

The perturbation in the deflagration to detonation transition process is investigated experimentally by utilizing one cavity and three successive cavities to induce weak and strong turbulences, respectively. The cavity serves as a "hot spot" in propagating deflagration , generating a pulse of shock waves locally and accelerating its velocity. The results suggest three modes of cavity perturbation on deflagration acceleration: direct transition to detonation, secondary acceleration to detonation after a long distance of steady propagation or mild decline in velocity, and failure to transition to detonation. This variation can primarily be attributed to various strengths of the precursor shock resulting from the acceleration of the flame by the cavity disturbance. The cavity perturbation must satisfy specific critical conditions to directly assist in the deflagration-to-detonation transition. Firstly, the escalated flame velocity due to the cavity perturbation must exceed the sound speed in combustion products . Secondly, the acceleration of the velocity rise must surpass specific critical values for the transition to detonation to be smoothly completed without a secondary acceleration.

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Publication Details

Journal
Combustion and Flame
Published
2024-12-19
DOI
https://doi.org/10.1016/j.combustflame.2024.113917
Citations
1
Primary Topic
Combustion and Detonation Processes
Type
article
Field-Weighted Citation Impact
1.30

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article

Experimental study of the perturbation of the cavity on the deflagration to detonation transition

Jian Li, Tianbao Ma, Deyao Wu
1 citations
Combustion and Flame
Combustion and Detonation Processes
1.30
article

Experimental study of the perturbation of the cavity on the deflagration to detonation transition

Jian Li, Tianbao Ma, Deyao Wu
article en
1 citations

Abstract

The perturbation in the deflagration to detonation transition process is investigated experimentally by utilizing one cavity and three successive cavities to induce weak and strong turbulences, respectively. The cavity serves as a "hot spot" in propagating deflagration , generating a pulse of shock waves locally and accelerating its velocity. The results suggest three modes of cavity perturbation on deflagration acceleration: direct transition to detonation, secondary acceleration to detonation after a long distance of steady propagation or mild decline in velocity, and failure to transition to detonation. This variation can primarily be attributed to various strengths of the precursor shock resulting from the acceleration of the flame by the cavity disturbance. The cavity perturbation must satisfy specific critical conditions to directly assist in the deflagration-to-detonation transition. Firstly, the escalated flame velocity due to the cavity perturbation must exceed the sound speed in combustion products . Secondly, the acceleration of the velocity rise must surpass specific critical values for the transition to detonation to be smoothly completed without a secondary acceleration.

Combustion and FlameVol. 273
Beijing Institute of Technology (CN)
National Natural Science Foundation of China
Climate action
Openalex Percentile: Top 11%
Combustion and Detonation Processes
1.30
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