Research Article  Open Access
V. A. Sabel'nikov, P. Bruel, "Determination of the Burning Velocity Domain of a Statistically Stationary Turbulent Premixed Flame in Presence of CounterGradient Transport", Journal of Combustion, vol. 2011, Article ID 821358, 7 pages, 2011. https://doi.org/10.1155/2011/821358
Determination of the Burning Velocity Domain of a Statistically Stationary Turbulent Premixed Flame in Presence of CounterGradient Transport
Abstract
The present study aims at providing a complete picture of the various propagation scenarios that a statistically stationary turbulent premixed flame may possibly undergo. By explicitly splitting the scalar turbulent flux between its gradient and countergradient contributions, the scalar governing equation is rewritten as an ordinary differential equation in the phase space. Then, an analysis of the characteristic equations in the vicinity of the reactants and products side is carried out. The domain of existence of the propagation velocity is then determined and positioned over the relevant Bray number range. It is shown in particular that when a countergradient transport at the cold leading edge of the flame is dominant, there still exists a possibility of observing a steady regime of propagation. This conclusion is compatible with recent experimental data and observations based on the analysis of direct numerical simulations.
1. Introduction
The determination of the burning velocity of turbulent premixed flames has been the subject of many experimental studies. As far as a given modelling of such reacting flows is concerned, the a priori value of for statistically stationary onedimensional turbulent flame is often estimated through the direct application of the results of the KolmogorovPetrovskiiPiskounov (KPP) theory [1] which showed that, for a onedimensional reaction zone without heat release described through the evolution of a single progress variable and with a constant diffusion coefficient , the steady propagation of the reaction zone is controlled by the behavior of the reaction rate at the reactants side and by the value of the diffusion coefficient. In many situations, experiments (Moss [2], Cheng and Shepherd [3], Troiani et al. [4], Zimmer et al. [5]) as well as direct numerical simulations (DNS) (Veynante et al. [6], Nishiki [7], Hauguel [8], Lee and Huh [9]) show that an expression of the turbulent transports via a gradient expression is not appropriate as some mechanisms may promote a transport with a sign identical to that of the mean scalar gradient. An extensive review of relevant experimental and DNS data can be found in the paper of Lipatnikov and Chomiak [10]. In such situations, the introduction of the Bray number proposed by Veynante et al. [6] proved to be helpful to discriminate between flow configurations featuring gradient turbulent flux (GTF) only ( or countergradient turbulent flux (CGTF) (.The Bray number was defined as where designates the heat release parameter and some order unity efficiency function which depends mainly on (and is an increasing function of) the ratio between the turbulence integral length scale and the flame thermal thickness. For , one of the most prominent mechanism leading to CGTF is directly related to the differential effect of the pressure gradient on the pockets of reactants (heavy) and products (lighter). But it should, nevertheless, be stressed, that even when such a mechanism is predominant, there still exists a gradient turbulent flux acting at scales much smaller than those of the pockets and for which the turbulent transport coefficient cannot be estimated through a turbulence model which integrates the whole turbulence scales. Accordingly, and following in that respect Veynante et al. [6], Zimont and Biagioli [11] or Lipatnikov and Chomiak [12], this suggests to consider the turbulent scalar flux as resulting from the competition between gradient and countergradient mechanisms.
Along these lines, we propose to study the propagation properties of a turbulent premixed flame by considering such a flux decomposition. First, an extended KPP analysis is developed. It combines all the possible scenarios with the change of and provides a general analysis whose results are not qualitatively dependent anymore on the modelling closures chosen but permit a clear and comprehensive discrimination between all the various propagation regimes.
We note that, in the framework of an eddybreakup model, an analytical attempt aimed at explaining the influence of the presence of CGTF on the turbulent flame propagation properties has been done by Corvellec et al. [13] who considered an idealized onedimensional premixed flame that propagates through highReynoldsnumber frozen turbulence. These authors dealt only with a flame brush formed by a GTF zone followed by a CGTF one. The scalar flux in each zone was expressed by employing a classical gradient formulation with the peculiarity of using a strictly negative diffusion coefficient for the CGTF zone. Thanks to this mathematical “trick”, it was then possible to employ the KPP technique to study the characteristics of the governing equation at both sides of the flame brush and at the intermediate point at which the flux is zero. This approach did not put into evidence a qualitative change in the nature of the burning velocity domain which appears to be still a semiinfinite interval. The lower bound though appeared to be controlled by both sides in such a situation. It drew also the attention on the fact that the KPP results cannot be extrapolated directly in such situations (in accordance to some extent with the numerical simulations of Bradley et al. [14]). The results of Corvellec et al. [13] cannot be considered as being of general implication since they are contingent to the recourse to an effective diffusion coefficient and are limited to the analysis of only one flame structure, that is, a GTF zone followed by a CGTF one. The Bray number is absent in the theory developed in [13] whereas DNS [6, 9] and recent experiments on turbulent premixed flames [4, 5] show that a different mean flame structure may be encountered that is, a CGTF zone followed by a GTF one. Thus, the present approach is more general than those followed previously since it permits to cover all the twozone mean flame structures that can be thought of. It shows in particular that as far as the burning velocity domain is concerned, qualitative differences with the KPP and Corvellec et al. [13] results are obtained.
2. Mathematical Formulation
2.1. Governing Equations
An unsteady 1D freely developing turbulent isenthalpic premixed flame is considered here and is described through the evolution of a single progress variable , where subscripts and denote the states of the reactant mixture and the fully burnt products, respectively, and defines the heat release parameter. Thus, in a fixed coordinate system the Favre averaged equation for and the continuity equation to be used later on, are given by is the turbulent flux, and is the mean reaction rate whose exact expression is not required at this stage. The flame is propagating from right to left, that is, .
We consider here the case for which countergradient mechanism is largely present in the flame as it is the case when the turbulence intensity is sufficiently low and/or the heat release parameter sufficiently large (see [6] for further details). Accordingly, the turbulent flux is expressed as represents the gradient contribution while corresponds to the countergradient part. Such a decomposition is compatible with the findings of Veynante et al. [6] who derived an algebraic expression for the flux as a function of the laminar flame velocity , the heat release parameter and the rms velocity , namely, . In this particular case, the countergradient contribution is equal to and the gradient one reads as
The ratio is just equivalent to the Bray number . If we introduce , where is the turbulence integral length scale and suppose that , then the gradient contribution can be classically written as . Here, the dependency of on the ratio between the flame thermal thickness and the turbulence integral length scale has been neglected. In the following analysis, we shall consider as given by (4) combined with a more general expression for , namely, where is a positive continuous function of such that . In the case of Veynante et al. [6], is a quadratic symmetric function, namely,
If we now rewrite the equation combined with the continuity equation, one obtains
It is worth noting that the analysis could be done also in the case, not considered here, where would be expressed without the introduction of a turbulent diffusion coefficient (e.g., using directly the decomposition of Veynante et al. [6]).
We rewrite (7) in a nondimensional form by defining the following reference parameters:(1)a velocity scale ,(2)a time scale ,(3)a length scale proportional to the integral turbulence scale, that is, ,(4)a reference turbulent diffusion coefficient ( is chosen in such a way that the proportionality coefficient between and is unity),(5)a flame velocity scale .
Thus, one has where , , , , , and . In the following and whenever unambiguous, we shall drop superscript *. So, with that convention, (8) reads as and the nondimensional form of the continuity equation (1) is given by
At this stage, it is important to underline that the form of (7) allows us to give a physical interpretation of the influence of CGTF on the flame structure (following mainly the reasoning adopted in [6]). The term of CGTF is a nonlinear convection term which tends to move both sides toward each other because of the change of sign of (positive at the fresh reactants side and then negative at the burnt products side). Such a “thinning” effect has to be counterbalanced by the gradient transport term in order to obtain a steady state flame propagation regime.
2.2. SteadyState Regime of Flame Propagation
Let us consider a steady state regime of flame propagation. Accordingly, in a coordinate system attached to the mean flame brush and introducing the flame mass consumption and the turbulent flame speed such as , the preceding continuity and progressvariable nondimensional equations are written as where .
We can rewrite (11) as a firstorder differential equation for on the domain , namely Introducing and , (12) is expressed as where denotes the derivation with respect to .
3. Analysis of the PEquation in the Vicinity of the Singular Points
Now, our primary objective is to determine the domain of existence of . In principle, we need for that to analyse the trajectories in the phase plane in the KPPlike manner. It is clear that a priori, due to the presence of the CGTF derivative , it is difficult to perform the KPP analysis in such a case.
Thus, leaving aside the question of determining the trajectories themselves, we focus on the determination of the associated domain by examining the characteristic equations of (13) at both sides of the brush. The implication of the relative position of and for the trajectories when they are tangent to the characteristics lines is also analyzed. We denote and and introduce the two functions and , such that for all but for which .(a)Reactants Side. In the limit and assuming that and ( and ), the characteristic equation associated with (13) is given by The required positiveness of the discriminant is assured as soon as . The corresponding roots and are both positive with . Accordingly, the reactants side is an improper unstable node and all the trajectories but one (the characteristic line itself) are tangent to the line. Two cases are to be considered in the vicinity of : (1) (the gradient contribution overcomes the countergradient one) and (2) the reverse situation prevails, that is, .(1) Gradient transport prevails, that is, . This implies that . Solving this inequality yields and . It is worth noting that when , one recovers the KPP domain.(2)Countergradient transport prevails, that is, . Two scenarios meet these inequalities, namely.(i). Solving this inequality yields and .(ii). This implies that for .
In both cases (1, 2), we must satisfy also Thus, for case 1 we have and for case 2 Using the definitions of , and , for case 1, one has or in equivalent form For case 2, we have Introducing the variables we can rewrite for case 1 and for case 2 It is important to note that relations in (23) are the sum of two sets, but not the product. Figure 1 illustrates the domain of existence of GTF and CGTF in the plane ( that followed from the analysis of (13) (for P) in the vicinity .(b)Products Side. In the limit and assuming that and ( and ), the characteristic equation associated with (13) is given by
The discriminant is always positive and there exists only one positive root . Accordingly, the products side is a saddle and all the trajectories are tangent to the line. Again, two situations are to be considered:(1)GTF prevails, that is, . This implies that or equivalently . In the limit , the original KPP behavior is recovered, that is, the absence of constraint.(2)CGTF prevails, that is, . This implies that or equivalently .
Using the relation we transform the above inequalities into the following form:
for case 1 (GTF)
for case 2 (CGTF) where Figures 2(a) and 2(b) present the domain of GTF and CGTF obtained from the analysis in the vicinity and for and , respectively. In the latter case, two remarkable values and of are introduced. They are defined by and .
(a)
(b)
There exists a maximum of four possible configurations, listed in Table 1, which correspond to the total turbulent flux behavior (gradient (G) or countergradient (CG)) in the vicinity of the singular points and .

Let us consider first the case . Analysis of inequalities (22)–(23) and (25)–(27) gives the following results.(i) G/G configuration: (ii)G/CG configuration is absent.(iii)CG/G configuration: (iv)CG/CG Configuration:
Domains of the above three possible configurations are given in Figure 3. Now for the case , all four configurations are possible, namely,(i) G/G configuration: Consequently, in this interval , we have .(ii)G/CG configuration:
for and for and again we have .(iii)CG/G configuration:
for with . In that case, we have .(iv) CG/CG configuration:
The different regions of the ( plane corresponding to these four configurations are presented in Figure 4. We note that the case is realised for the classical eddybreakup model where and if , Veynante et al. case [6]. In that case, one has and consequently and . Thus, The case is obtained if where is some positive contant. So we have For Veynante et al. [6], and so
It should be noted that experimental data [3, 15] suggest that is shifted towards the burnt gas side. Such a situation can be modelled by relation (36) with , and, in this case, we can have . As was shown previously, in such a situation, the configuration G/CG is absent. Such a result is compatible with DNS results for 1D freely propagating turbulent premixed flame [6, 9]. It is also in correspondance with the recent experimental data of Troiani et al. [4] who investigated bluffbody stabilized turbulent premixed flames. These authors showed that the radial component of the scalar flux (which is the counterpart of ) could exhibit a transition between a countergradient to a gradient behavior when moving along the normal to the mean front from reactants toward products.
4. A Particular Configuration: The Murray's Equation
The Murray's equation [16] is a good example of the convectiondiffusion equation, of the type considered here, to demonstrate that the common viewpoint that at the leading edge it is the diffusion term which always drives the flame propagation is not universal. Such an equation is obtained as a particular case of (9) corresponding to , , , and . In such a case, we have , , and . We note that formally though, corresponds to leading to . But we will consider here like a parameter not linked to . In such a situation, by denoting and , (11) reduced to that analyzed by Murray [16] to determine the wave speed , namely, Murray [16] showed that travelling wave solutions exist for all where or equivalently with our notations Thus, it appears that in that particular case, for and in the zone , it is the countergradient transport that prevails (see the domain CG/G in Figures 3 and 4).
5. Concluding Remark
A methodology that permits to study the domain of the tubulent flame velocities for a steady regime of a turbulent premixed flame propagation has been presented. It has been shown how the introduction of the parameter (defined by 32) that combines both the countergradient flux and the mean reaction rate behavior at both edges of the flame can be used to determine the domain where a steady regime of propagation may exist for any combination of scalar fluxes that dominate at the flame edges. It is worth noticing though that the present analysis of the sole velocity domain does not prove the existence/unicity of the steady solutions. Consequently, future work will concentrate on the use of numerical simulations to study these questions.
Acknowledgments
The support of the first author by ONERA as well as the support of the second author by CNRS are greatly acknowledged.
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Copyright
Copyright © 2011 V. A. Sabel'nikov and P. Bruel. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.