2013
DOI: 10.1137/120864891
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Spectral Behavior of Combustion Fronts with High Exothermicity

Abstract: We study fronts in a reaction-diffusion model for high Lewis number combustion processes with the reaction rate in the form of an Arrhenius law. By a combination of spectral energy estimates and Evans function computation, we study the unstable spectrum of a class of combustion fronts with high exothermicity, where the previously known results do not apply and interesting spectral behavior is observed.

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Cited by 9 publications
(13 citation statements)
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“…The Evans function is an analytic function of the spectral parameter defined in some region of the complex plane. It was used for example in the context of nerve impulse equations [1,9,20,39], pulse solutions to the generalized Korteveg-de Vries, Benjamin-Bona-Mahoney and Boussinesq equations [28], multi-pulse solutions to reaction-diffusion equations [2,3], solutions to perturbed nonlinear Schrödinger equations [21,22,24], near integrable systems [25], traveling hole solutions of the one-dimensional complex Ginzburg-Landau equation near the Nonlinear-Schrödinger limit [23], and in the context of combustion problems [4,12,18]. The Evans function can be expressed in several different ways depending on the size of the stable and unstable manifolds of the linear system.…”
mentioning
confidence: 99%
“…The Evans function is an analytic function of the spectral parameter defined in some region of the complex plane. It was used for example in the context of nerve impulse equations [1,9,20,39], pulse solutions to the generalized Korteveg-de Vries, Benjamin-Bona-Mahoney and Boussinesq equations [28], multi-pulse solutions to reaction-diffusion equations [2,3], solutions to perturbed nonlinear Schrödinger equations [21,22,24], near integrable systems [25], traveling hole solutions of the one-dimensional complex Ginzburg-Landau equation near the Nonlinear-Schrödinger limit [23], and in the context of combustion problems [4,12,18]. The Evans function can be expressed in several different ways depending on the size of the stable and unstable manifolds of the linear system.…”
mentioning
confidence: 99%
“…However, we have the lingering issue of translation invariance: that the equation (2.2) is translation invariant and that the above projective boundary conditions do not fix a particular translate. To resolve this, we use a trick from [12] that allows us to specify a particular function value in the "middle" of the region in exchange for doubling the dimension of the problem. Specifically, that if (2.2) when written as a system is ∂ z y = F (y), then we introduce the variableỹ with ∂ zỹ = −F (ỹ) so rather than working on the region [−L, L], y is the solution on [0, L] andỹ is the solution running backwards on [−L, 0].…”
Section: Numerical Existence Studymentioning
confidence: 99%
“…We numerically compute these integrals to locate zeroes of the Evans function in a given domain. Generally, this technique is known as the method of moments [15,41,42]. However, since in our case we are only looking for one root at a time only, the use of the higher moments (where z is replaced by z n ) is not necessary.…”
Section: Linear Stabilitymentioning
confidence: 99%
“…Front solution of the system(15) in the case c = 1.8588, ε = 0.1, h = 0.3, σ = 0.25, δ = 0.0005, and T ign = 0.01, and Z = 6. The solid line corresponds to u, the dashed line to y, and the dotted line to z.…”
mentioning
confidence: 99%