2020
DOI: 10.1016/j.fuel.2020.117110
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Modelling of flammable fuels in small and large scale turbulent environments

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Cited by 4 publications
(3 citation statements)
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“…This discrepancy in the time needed to reach the peak pressure is a result of using the present flame surface density model. A recent parametric study by the present author [47] indicated that this discrepancy can simply be eliminated by varying the initial progress variable set to numerically ignite the mixture inside the chamber.…”
Section: Resultsmentioning
confidence: 87%
“…This discrepancy in the time needed to reach the peak pressure is a result of using the present flame surface density model. A recent parametric study by the present author [47] indicated that this discrepancy can simply be eliminated by varying the initial progress variable set to numerically ignite the mixture inside the chamber.…”
Section: Resultsmentioning
confidence: 87%
“…A is the model constant, the default value given by Zimont [12] is 0.52 and was later reduced to 0.38 following Yehia & Abdel-Raheem [13] , 𝑢′ is the root mean square velocity, S is the laminar flame speed, l t is turbulence length scale, τ l /𝑢′ is the turbulent time scale and τ α/ S is the chemical time scale.…”
Section: Combustion Modellingmentioning
confidence: 99%
“…A is the model constant, the default value given by Zimont [41] is 0.52 and was later reduced to 0.38 following Yehia & Abdel-Raheem [42], 𝑢′ is the root mean square velocity, S 𝑙 is the laminar flame speed, lt is turbulence length scale, τ 𝑡 = l 𝑡 /𝑢′ is the turbulent time scale and τ 𝑐 = α/ S 𝑙 2 is the chemical time scale.…”
Section: Combustion Modelingmentioning
confidence: 99%