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Astron. Astrophys. 324, 161-176 (1997)
6. Concluding remarks
The non-linear multigrid methods developed in this paper for
multilevel RT applications are characterized by a very high
convergence speed that does not deteriorate when the grid resolution
is refined. For this reason they are particularly suitable for solving
complicated 1D, 2D or 3D multilevel problems, where grid-sizes smaller
than about 10 km are required. The computational work one can save by
using the non-linear multigrid RT method instead of the operator
splitting methods currently in use (like, e.g., the MALI scheme), is
the larger the smaller the grid-size. This saving is larger for 3D
applications than for 2D, which, in turn, is larger than for 1D.
Our nested multigrid RT code is even more effective. Its storage
requirements are only a factor larger than
those of the MALI method of Paper I (with for
1D, for 2D, and for 3D
applications), and it is a factor 2 faster than the standard
multigrid RT technique. It, thus, allows the accurate solution of RT
problems with a computational effort equal to the cost of only
very few formal solutions of the RT equation. For instance, if
n indicates the number of grid-points per decade, the
computational work of the Jacobi-type MALI scheme of Paper I scales
approximately as , the MUGA method of Trujillo
Bueno & Fabiani Bendicho (1995; 1996) (which is based on
Gauss-Seidel iterations) as , their SOR-based
technique as , while the multilevel RT
multigrid methods presented here scale as n, because the
very high convergence rate of the multigrid iteration is insensitive
to the grid-size, while the cost per MG iteration scales as n.
To our knowledge there is presently no other multilevel transfer code
capable of offering this very high performance in scalar-class
computers. Preliminary results indicate that a similarly good relative
improvement is obtained in calculations for realistic atomic models
and atmospheres, whose presentation we leave for future
publications.
© European Southern Observatory (ESO) 1997
Online publication: May 26, 1998
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