2018
DOI: 10.1016/j.combustflame.2018.03.006
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Deflagration-to-detonation transition in an unconfined space

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Cited by 28 publications
(10 citation statements)
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“…Here n s -number of species, ρ -density of the mixture, T -temperature, P -thermodynamic pressure, R 0 -ideal gas constant, c i -concentration of species i, X i -molar fraction, h i -specific molar enthalpy, j d i -molar diffusion flux, µ -shear viscosity of the mixture, λ -thermal conductivity of the mixture,ω i -chemical source of species i, W i -molar mass, Σ -flame folding factor. The thickness of the temperature profile l is chosen such that a minimal ignition energy is provided [24]. Note that equations (2.3) and (2.5) imply the conventional continuity equation, ∂ρ/∂t + ∂ρu/∂x = 0.…”
Section: Mathematical Modelmentioning
confidence: 99%
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“…Here n s -number of species, ρ -density of the mixture, T -temperature, P -thermodynamic pressure, R 0 -ideal gas constant, c i -concentration of species i, X i -molar fraction, h i -specific molar enthalpy, j d i -molar diffusion flux, µ -shear viscosity of the mixture, λ -thermal conductivity of the mixture,ω i -chemical source of species i, W i -molar mass, Σ -flame folding factor. The thickness of the temperature profile l is chosen such that a minimal ignition energy is provided [24]. Note that equations (2.3) and (2.5) imply the conventional continuity equation, ∂ρ/∂t + ∂ρu/∂x = 0.…”
Section: Mathematical Modelmentioning
confidence: 99%
“…In computations it is implemented by detailed study of the hot spot width l for different values of Σ such that minimising the chosen value of width of the hot spot by 5% leads to an ignition failure. The system is then integrated for different constant values of Σ and internal structure of the accelerating flame front is investigated (for details see [24]). As it was predicted and was shown in a number of works [16,24] there is a critical value of Σ leading to very strong DDT, when an over-driven detonation is formed.…”
Section: Numerical Implementationmentioning
confidence: 99%
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“…This is primarily due to the practical importance of studies of the stability for flames subjected to small perturbations: it is instability that is the main cause of flame autoturbulization [2,3] and acceleration [4,5]. In turn, acceleration of the flame can cause its transition to detonation [6][7][8] or to deflagration explosion [9]. Thus, the problem of hydrodynamic flame stability is closely related to the general problem of explosion safety [9][10][11].…”
Section: Introductionmentioning
confidence: 99%