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Development and Verification of Nuclear Calculation Methods for ...

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-23-<br />

4. 3. The TWODIM Programme<br />

The fundamental methods outlined above <strong>for</strong>m the basic principles in<br />

the two-dimensional (XY, RZ, R8), multi-group (maximum 20 groups<br />

<strong>for</strong> 25 x 25 meshes) finite difference equation computer programme<br />

TWODIM. The programme was especially designed <strong>for</strong> the detailed<br />

determination <strong>of</strong> flux <strong>and</strong> power distributions in light-water fuel element<br />

assemblies with a detailed treatment <strong>of</strong> control rods <strong>and</strong> water gaps as<br />

shown in fig. 13.<br />

A flux representation where the fluxes were assigned to the midpoints<br />

instead <strong>of</strong> the intersections <strong>of</strong> the mesh lines was chosen. This is<br />

enormously advantageous <strong>for</strong> particular multi-group problems, where the<br />

scattering terms in equation (4. 6) have smaller storage requirements.<br />

Reaction rates are determined quite exactly by means <strong>of</strong> this English method,<br />

whereas the leakage seems to be less precisely determined than with the<br />

American one. Furthermore, the leakage constitutes only part <strong>of</strong> the total<br />

neutron balance.<br />

Boundary conditions either in the shape <strong>of</strong> full gamma matrices or the<br />

conventional diagonal terms may be obtained from the HECS programme<br />

(ref. 15).<br />

A successive overrelaxation method, SOR, or a successive line overrelaxation<br />

method, SLOR, is applied <strong>for</strong> the inner iterations with the best<br />

relaxation factor found. In the SLOR method blocks <strong>of</strong> horizontal or vertical<br />

lines <strong>of</strong> mesh points may be solved simultaneously in a numerically<br />

stable way by means <strong>of</strong> a tridiagonal <strong>for</strong>ward elimination <strong>and</strong> backward substitution<br />

method. This direct method <strong>for</strong> the subproblem implies no appreciable<br />

further arithmetic ef<strong>for</strong>ts compared with the usual point relaxation<br />

scheme <strong>and</strong> it generally gains a factor <strong>of</strong> V"2~ in convergence rate. More<br />

impresrive gains can be achieved, especially in problems with non-uni<strong>for</strong>m<br />

mesh spacings.<br />

The extension <strong>of</strong> the method to greater blocks <strong>of</strong> subproblem« is described<br />

in ref. 16 . The spectral radius <strong>for</strong> the block Jacobi iterative matrix<br />

does indeed decrease as more points are improved simultaneously,<br />

which gives a greater (asymptotic) convergence rate (per iteration). However,<br />

the increased computational ef<strong>for</strong>ts per iteration <strong>and</strong> associated numerical<br />

difficulties due to dangerous accumulation <strong>of</strong> rounding-<strong>of</strong>f errors<br />

seem to make the method leas advantageous.<br />

As the spectral radius ji(B) <strong>for</strong> the block Jacobi matrix approaches<br />

unity, the accurate determination <strong>of</strong> «_ becomes more important as can

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