Gray-Scott Reaction-Diffusion Cell with an Applied Electric Field

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Consider the Gray–Scott reaction-diffusion cell with an applied electric field. The governing equations and boundary and initial conditions are:
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Contributed by: Housam Binousand Brian G. Higgins (June 2013)
Open content licensed under CC BY-NC-SA
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Details
In the discrete Chebyshev–Gauss–Lobatto case, the interior points are given by . These points are the extrema of the Chebyshev polynomials of the first kind,
.
The Chebyshev derivative matrix at the quadrature points is an
matrix
given by
,
,
for
, and
for
and
,
where for
and
.
The matrix is then used as follows:
and
, where
is a vector formed by evaluating
at
,
, and
and
are the approximations of
and
at the
.
Reference
[1] P. Moin, Fundamentals of Engineering Numerical Analysis, Cambridge, UK: Cambridge University Press, 2001.
[2] L. N. Trefethen, Spectral Methods in Matlab, Philadelphia: SIAM, 2000.
[3] A. W. Thornton and T. R. Marchant, "Semi-analytical solutions for a Gray–Scott reaction–diffusion cell with an applied electric field," Chemical Engineering Science, 63(2), 2008 pp. 495–502. DOI: 10.1016/j.ces.2007.10.001 .
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