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Even though each of the equations only involves first order
derivatives, simple backward or forward differences are not
suitable for integration of three dimensional scalar fields.
Gauss-Seidel requires a diagonally-dominant system for assured
convergence. Though forward and backward finite differences
will generally converge, a simple combination of both schemes
will reduce the magnitude of the off-diagonal terms and thus
guarantee convergence. In addition, this provides a set of
difference equations which are symmetric with respect to grid
traversal directions. First, some notational conventions:
The photon flux equation has the following finite
difference relationships:
or,
Similarly, the ion production equation can be expressed as a finite
difference equation.
So that,
And finally,
The free boundaries of the system (top and bottom ion boundaries
and the daylight bottom and nighttime top flux boundaries) can
easily be handled by extrapolating to virtual grid points beyond the
boundaries and using the same difference equations. The virtual
points, of course, are not integrated.
Next: Integration Solver Selection
Up: Integration Scheme
Previous: Integration Grid Definition
Carlos A Cruz
10/27/1997