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Physica A
journal homepage: www.elsevier.com/locate/physa
Generalized analytical expressions for the burning velocity in a
combustion model with non-constant transport coefficients and several
specific heats
Toni Pujol
a,∗
, Joaquim Fort
b
, Lino Montoro
a
, Joan J. Suñol
b
a
Dept. d’Enginyeria Mecànica i de la Construcció Industrial, Escola Politècnica Superior, Universitat de Girona, Campus Montilivi, 17071 Girona, Catalonia, Spain
b
Dept. de Física, Escola Politècnica Superior, Universitat de Girona, Campus Montilivi, 17071 Girona, Catalonia, Spain
article info
Article history:
Received 7 April 2009
Received in revised form 10 July 2009
Available online xxxx
Keywords:
1D combustion model
Bounds for the propagation speed
Premixed laminar flame
Reaction–diffusion model
abstract
We derive new expressions to estimate the burning velocity of a laminar gas flame
in a simplified combustion model based on a one-step single reaction with transport
coefficients (mass and heat) depending on temperature, and species with different specific
heats. These new expressions generalize the bounds and approximations previously
derived by Williams, von Karman, Zeldovich and Frank–Kamenetskii, Benguria and
Depassier, and the matching asymptotic expansion method in a two zone model. The
comparison of the flame speed predicted by these new analytical expressions with that
numerically simulated by the full combustion model for a large variety of cases allows
us to determine their range of validity. The upper bound based on the Benguria and
Depassier method provides very good approximations for the actual propagation speed
of combustion flames, being substantially better than the asymptotic method used in the
recent papers.
© 2009 Elsevier B.V. All rights reserved.
1. Introduction
In laminar flame theory, the combustion of premixed gases with no energy losses develops a flame front that propagates
at a constant speed [1,2]. Classical analyses carried out by several investigators (e.g., Refs. [3–5]) have provided well-known
analytical expressions for predicting this laminar burning velocity on simplified combustion models. Although currently
thought of having limited interest, some of these methods are still in use when investigating the essence of realistic
combustion processes. A very recent example may be the analysis of the propagation of laminar premixed flames with a
reversible reaction term [6]. Analytical approaches are also useful, as a first step, to test numerical codes before introducing
more complicated effects (e.g., heat losses) that make analytical estimations of the flame speed impossible.
Most well-known analytical expressions usually adopt a simplified one-dimensional (1D) model of a unimolecular binary
mixture with a single-step reaction, with background flow at rest and with constant transport coefficients and specific heats.
Some attempts to generalize these expressions to more realistic conditions have been carried out, although focusing in one
particular methodology applied to solve a specific combustion problem (see, e.g., Refs. [7–10]). In contrast, the purpose
of the present paper is to discuss the validity of a wide range of methodologies for estimating the burning velocity in a
1D combustion model that takes account of (1) the temperature dependence of mass and heat diffusivities and (2) the
differences of specific heats between reactants and products. In addition, our model takes into consideration the very realistic
case of including a non-zero flow velocity across the flame front due to density variations (see, e.g., Ref. [11]). Note that this
effect has not been included in the recent studies focused on derived analytical expressions for the wavefront speed of
combustion flames [1,2,5,8,9].
∗
Corresponding author.
E-mail address: toni.pujol@udg.edu (T. Pujol).
0378-4371/$ – see front matter © 2009 Elsevier B.V. All rights reserved.
doi:10.1016/j.physa.2009.08.016
Please cite this article in press as: T. Pujol, et al., Generalized analytical expressions for the burning velocity in a combustion model with non-constant
transport coefficients and several specific heats, Physica A (2009), doi:10.1016/j.physa.2009.08.016