Physics:Majda's model

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Majda's model is a qualitative model (in mathematical physics) introduced by Andrew Majda in 1981 for the study of interactions in the combustion theory of shock waves and explosive chemical reactions.[1]

The following definitions are with respect to a Cartesian coordinate system with 2 variables. For functions [math]\displaystyle{ u(x,t) }[/math], [math]\displaystyle{ z(x,t) }[/math] of one spatial variable [math]\displaystyle{ x }[/math] representing the Lagrangian specification of the fluid flow field and the time variable [math]\displaystyle{ t }[/math], functions [math]\displaystyle{ f(w) }[/math], [math]\displaystyle{ \phi (w) }[/math] of one variable [math]\displaystyle{ w }[/math], and positive constants [math]\displaystyle{ k, q, B }[/math], the Majda model is a pair of coupled partial differential equations:[2]

[math]\displaystyle{ \frac{\partial u(x,t)}{\partial t} + q \cdot \frac{\partial z(x,t)}{\partial t} + \frac{\partial f(u(x,t))}{\partial x} = B \cdot \frac{\partial^2u(x,t)}{\partial x^2} }[/math]
[math]\displaystyle{ \frac{\partial z(x,t)}{\partial t} = - k \cdot \phi (u(x,t)) \cdot z(x,t) }[/math][2]
the unknown function [math]\displaystyle{ u = u(x,t) }[/math] is a lumped variable, a scalar variable formed from a complicated nonlinear average of various aspects of density, velocity, and temperature in the exploding gas;
the unknown function [math]\displaystyle{ z = z(x,t) \in [0,1] }[/math] is the mass fraction in a simple one-step chemical reaction scheme;
the given flux function [math]\displaystyle{ f = f(w) }[/math] is a nonlinear convex function;
the given ignition function [math]\displaystyle{ \phi = \phi (w) }[/math] is the starter for the chemical reaction scheme;
[math]\displaystyle{ k }[/math] is the constant reaction rate;
[math]\displaystyle{ q }[/math] is the constant heat release;
[math]\displaystyle{ B }[/math] is the constant diffusivity.[2]
Since its introduction in the early 1980s, Majda's simplified "qualitative" model for detonation ... has played an important role in the mathematical literature as test-bed for both the development of mathematical theory and computational techniques. Roughly, the model is a [math]\displaystyle{ 2 \times 2 }[/math] system consisting of a Burgers equation coupled to a chemical kinetics equation. For example, Majda (with Colella & Roytburd) used the model as a key diagnostic tool in the development of fractional-step computational schemes for the Navier-Stokes equations of compressible reacting fluids ...[3]

References

  1. Majda, Andrew (1981). "A qualitative model for dynamic combustion". SIAM J. Appl. Math. 41 (1): 70–93. doi:10.1137/0141006. 
  2. 2.0 2.1 2.2 Humphreys, Jeffrey; Lyng, Gregory; Zumbrun, Kevin (2013). "Stability of viscous detonations for Majda's model". Physica D: Nonlinear Phenomena 259: 63–80. doi:10.1016/j.physd.2013.06.001. Bibcode2013PhyD..259...63H. 
  3. Lyng, Gregory D. (2015). Spectral and nonlinear stability of viscous strong and weak detonation waves in Majda's qualitative model. http://www.icders.org/ICDERS2015/abstracts/ICDERS2015-283.pdf.