2016
DOI: 10.1080/13647830.2016.1249523
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The role of spontaneous waves in the deflagration-to-detonation transition in submillimetre channels

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Cited by 49 publications
(14 citation statements)
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“…It is known [12] that for a flame propagating in a tube with no-slip walls viscous dissipation in the flow ahead of the advancing flame heats the gas mixture increasing the temperature in the boundary layer by 150-200K higher than the gas temperature in the bulk flow near the tube axis. According to simulations of the flame propagating in submillimetre two-dimensional channels with a one-step model [49][50][51][52] viscous heating in the boundary layer induces local explosions near the boundary, which in turn leads to DDT. In simulations using a one-step model, this leads to the autoignition producing a spontaneous wave, which occurs during the time about 10 µs for submillimetre channels (about 60 µs for 2cm channel) that elapse between the passage of the precursor shock and the flame arrival.…”
Section: Discussionmentioning
confidence: 99%
“…It is known [12] that for a flame propagating in a tube with no-slip walls viscous dissipation in the flow ahead of the advancing flame heats the gas mixture increasing the temperature in the boundary layer by 150-200K higher than the gas temperature in the bulk flow near the tube axis. According to simulations of the flame propagating in submillimetre two-dimensional channels with a one-step model [49][50][51][52] viscous heating in the boundary layer induces local explosions near the boundary, which in turn leads to DDT. In simulations using a one-step model, this leads to the autoignition producing a spontaneous wave, which occurs during the time about 10 µs for submillimetre channels (about 60 µs for 2cm channel) that elapse between the passage of the precursor shock and the flame arrival.…”
Section: Discussionmentioning
confidence: 99%
“…One mechanism involves viscous heating of the boundary layers in the flow induced by the precursor shock that forms ahead of the flame. The shock and viscous dissipation can heat the reactive material in the boundary layer to a condition where autoignition can occur in the time between the passage of the shock and the arrival of the flame [5][6][7][8]. Another mechanism involves localized pressure increases near the flame, which enhances the local burning rate, which, in turn, leads to further local pressure increases.…”
Section: Introductionmentioning
confidence: 99%
“…The channel had a diameter of 17.4 cm and blockage ratio br = 0.3 to match the experimental configuration of Kuznetsov [31]. Figure 6 shows reaction front position vs. reaction front speed for these simulations using FAST (Flame Acceleration Simulation Tool) [35], in which the mesh was dynamically refined around shocks, flame fronts and in regions of large gradients of density, pressure or composition. In addition to the simulation results, Fig.…”
Section: Comparison Between Ga-nm Graphical Approach and Experimentamentioning
confidence: 99%