Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow

Based on purely geometrical considerations of the level sets of the scalar G ( x , t ) satisfying the field equation ( G - equation), A. Kerstein, T. Ashurst and F. Williams [Phys. Rev. A, 37 , 2728, (1988)] derived the expression for the mean flame consumption velocity in a 1D premixed turbulent fl...

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Main Authors: Vladimir A. Sabelnikov, Alan R. Kerstein
Format: Article
Language:English
Published: SAGE Publishing 2012-03-01
Series:International Journal of Spray and Combustion Dynamics
Online Access:https://doi.org/10.1260/1756-8277.4.1.61
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spelling doaj-ccd87d2dcd4247b591fe84e61af0d8a72020-11-25T02:54:19ZengSAGE PublishingInternational Journal of Spray and Combustion Dynamics1756-82771756-82852012-03-01410.1260/1756-8277.4.1.6110.1260_1756-8277.4.1.61Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent FlowVladimir A. Sabelnikov0Alan R. Kerstein1 ONERA, The French Aerospace Lab, F-91761 Palaiseau, France Combustion Research Facility, Sandia National Laboratories, Livermore, California 94551-0969Based on purely geometrical considerations of the level sets of the scalar G ( x , t ) satisfying the field equation ( G - equation), A. Kerstein, T. Ashurst and F. Williams [Phys. Rev. A, 37 , 2728, (1988)] derived the expression for the mean flame consumption velocity in a 1D premixed turbulent flame in a homogeneous flow of uniform density in terms of the volume average of |▽ G ( x , t )| for a particular choice of the initial condition G ( x , t = 0). In the present study we develop further the KAW work in two directions. First, in section 2, in contrast with the KAW approach, we consider the G - equation immediately and, using ensemble averaging, obtain the expression for the mean flame consumption velocity in terms of ensemble averages equivalent to the KAW result. Then, in section 3 the developed approach is applied to the case of homogeneous turbulent flow with a uniform mean strain rate field depending only on time.https://doi.org/10.1260/1756-8277.4.1.61
collection DOAJ
language English
format Article
sources DOAJ
author Vladimir A. Sabelnikov
Alan R. Kerstein
spellingShingle Vladimir A. Sabelnikov
Alan R. Kerstein
Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
International Journal of Spray and Combustion Dynamics
author_facet Vladimir A. Sabelnikov
Alan R. Kerstein
author_sort Vladimir A. Sabelnikov
title Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
title_short Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
title_full Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
title_fullStr Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
title_full_unstemmed Derivation from the Field Equation of the Mean Consumption Velocity for Front Propagation in Homogeneous Turbulent Flow
title_sort derivation from the field equation of the mean consumption velocity for front propagation in homogeneous turbulent flow
publisher SAGE Publishing
series International Journal of Spray and Combustion Dynamics
issn 1756-8277
1756-8285
publishDate 2012-03-01
description Based on purely geometrical considerations of the level sets of the scalar G ( x , t ) satisfying the field equation ( G - equation), A. Kerstein, T. Ashurst and F. Williams [Phys. Rev. A, 37 , 2728, (1988)] derived the expression for the mean flame consumption velocity in a 1D premixed turbulent flame in a homogeneous flow of uniform density in terms of the volume average of |▽ G ( x , t )| for a particular choice of the initial condition G ( x , t = 0). In the present study we develop further the KAW work in two directions. First, in section 2, in contrast with the KAW approach, we consider the G - equation immediately and, using ensemble averaging, obtain the expression for the mean flame consumption velocity in terms of ensemble averages equivalent to the KAW result. Then, in section 3 the developed approach is applied to the case of homogeneous turbulent flow with a uniform mean strain rate field depending only on time.
url https://doi.org/10.1260/1756-8277.4.1.61
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