1996
DOI: 10.1016/0010-2180(95)00195-6
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On the “tulip flame” phenomenon

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Cited by 405 publications
(230 citation statements)
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“…3(b). The calculation grid is modified periodically in the course of calculation, so that the sizes and positions of all domains in rate increases by order of magnitude in the process of precursor acceleration [29,30]. As a result, quite quickly the Mach number Ma lab becomes comparable to unity.…”
Section: Basic Equations Of the Direct Numerical Simulationsmentioning
confidence: 99%
“…3(b). The calculation grid is modified periodically in the course of calculation, so that the sizes and positions of all domains in rate increases by order of magnitude in the process of precursor acceleration [29,30]. As a result, quite quickly the Mach number Ma lab becomes comparable to unity.…”
Section: Basic Equations Of the Direct Numerical Simulationsmentioning
confidence: 99%
“…There are also other opinions on the tulipflame formation mechanism. According to some of them, the formation of the tulip flame is a manifestation of Taylor instability driven by the deceleration of the flame tip (Clanet and Searby, 1996).…”
Section: Closed-tube Combustionmentioning
confidence: 99%
“…In most simulation runs, thermal expansion was chosen as 8   , which is typical for the burning of alkane hydrocarbons. However, other expansion factors 16 …”
Section: Direct Numerical Simulationsmentioning
confidence: 99%
“…flame interaction with turbulent vortices [8][9][10][11], intrinsic flame instabilities [2,[12][13][14][15], ignition peculiarities [16,17], flame-acoustic interactions [18,19], etc. It is however noted that, for flames in tubes/channels, the role of turbulence and flame instabilities is rather supplementary as compared to either the Shelkin mechanism in smooth tubes [3,7,[20][21][22][23][24] or acceleration in tubes with obstacles [25,26].…”
Section: Introductionmentioning
confidence: 99%