We consider an initial-value problem based on a class of scalar nonlinear hyperbolic reaction–diffusion equations of the general form uτ τ + uτ = uxx + ε(F(u) + F(u)τ ), in which x and τ represent dimensionless distance and time, respectively, and ε > 0 is a parameter related to the relaxation time. Furthermore, the reaction function, F(u), is given by the Arrhenius combustion nonlinearity, F(u) = e−E/u(1 − u), in which E > 0 is a parameter related to the activation energy. The initial data are given by a simple step function with u(x, 0) = 1 for x ≤ 0 and u(x, 0) = 0 for x > 0. The above initial-value problem models, under certain simplifying assumptions, combustion waves in premixed gaseous fuels; here, the variable u represents the non-dimensional temperature. It is established that the large-time structure of the solution to the initial-value problem involves the evolution of a propagating wave front, which is of reaction–diffusion or reaction–relaxation type depending on the values of the problem parameters E and ε

Item Type:	Refereed Article
Keywords:	hyperbolic reaction equations; relaxation; Arrhenius combustion
Research Division:	Mathematical Sciences
Research Group:	Applied mathematics
Research Field:	Theoretical and applied mechanics
Objective Division:	Expanding Knowledge
Objective Group:	Expanding knowledge
Objective Field:	Expanding knowledge in the mathematical sciences
UTAS Author:	Bassom, AP (Professor Andrew Bassom)
ID Code:	154909
Year Published:	2022
Deposited By:	Mathematics
Deposited On:	2023-01-18
Last Modified:	2023-02-08
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