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Discretisation of a convection-diffusion equation
K W Morton,
I J Sobey
Revised September 1991.
The unsteady convection diffusion equation with constant velocity
admits an exact solution in the form of a convolution integral of the
concentration at an earlier time and a travelling exponential
function. This representation can be put in the form of an evolution
operator relating the solution at one time level to that at a previous
time level. By using this evolution operator we are able to unify many
numerical schemes for the convection diffusion equation, showing
inter-relationships between finite difference and finite element
schemes and presenting a general framework for further error analysis.
In particular the Lax Wendroff approximation arises from the evolution
of a quadratic approximation to the initial distribution, and Leonard's
QUICKEST scheme comes both from evolving a cubic approximation to the
initial distribution and also from a finite element solution using a
mixed norm and piecewise linear basis functions. The Peano kernel
theorem is used to derive error bounds for these two methods; Fourier
analysis is used to obtain practical stability regions and further
insight into their accuracy.
Finally, it has long been conjectured that there should be a connection
between the optimal test functions that arise in the application of
Petrov-Galerkin methods to the steady convection diffusion equation and
the test functions arising in finite element approximations to the
unsteady advection equation. We prove a direct relationship in the
case of a particular mixed norm.
- Key words and phrases:
- Convection-diffusion, Lax Wendroff, QUICKEST,
finite differences, finite elements, optimal test functions
The work reported here forms part of the research programme of the
Oxford-Reading
Institute for Computational Fluid Dynamics.
This paper is not currently available electronically.
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