Majda's model explained
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
,
of one spatial variable
representing the
Lagrangian specification of the fluid flow field and the
time variable
, functions
,
of one variable
, and positive constants
, the
Majda model is a pair of coupled
partial differential equations:
[2]
+q ⋅
+
| \partialf(u(x,t)) |
\partialx |
=B ⋅
| \partial2u(x,t) |
\partialx2 |
=-k ⋅ \phi(u(x,t)) ⋅ z(x,t)
[2] the unknown function
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
is the
mass fraction in a simple one-step chemical reaction scheme;
the given flux function
is a nonlinear convex function;
the given ignition function
is the starter for the chemical reaction scheme;
is the constant
reaction rate;
is the constant heat release;
is the constant
diffusivity.
[2] Notes and References
- Majda, Andrew. A qualitative model for dynamic combustion. SIAM J. Appl. Math.. 41. 1. 70–93. 10.1137/0141006. 1981.
- Humphreys, Jeffrey. Lyng, Gregory. Zumbrun, Kevin. Stability of viscous detonations for Majda's model. Physica D: Nonlinear Phenomena. 259. 2013. 63–80 . 1301.1260. 10.1016/j.physd.2013.06.001. 2013PhyD..259...63H. 119301730.