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The system also allows you to refine your model by adding (or removing) cuts if the final error checking yields unacceptable results.

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The system will always correctly compute the average behavior over the region, you will just loose the axial shape, and true two dimensional equivalence will no longer be achieved.

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label (str) – Name used to identify the section. It will be used to identify the cut on the command line. It is recommended to use a unique tag no longer than 12 characters.

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label (str) – Name used to identify the section. It will be used to identify the cut on the command line. It is recommended to use a unique tag no longer than 12 characters.

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Each cut reference returned by parameters.add_cut and parameters.add_axial_reflector_cut has the following methods to access and modify data:

For axial sections that do not contain source (fissionable) material, the following method is used to define the homogenization calculation.

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will homogenize a 6 cm region above the active core. Equivalence and replacement tests are not available for these cuts.

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The specification of a cut includes a height, that is, homogenization is not performed on a true plane cut, but rather an axial section. A two dimensional calculation is emulated by placing reflective boundary conditions on the top and bottom planes, but it will only be truly two dimensional if there are no axial changes within the section. Since nodal equivalence currently only covers the radial plane, with axial leakage assumed to be zero, it is best to try and limit the amount of axial heterogeneity within your sections. This only applies to cuts containing active (fissionable) material, as reflector regions are treated differently. However, especially in research reactors, there are frequently a lot of axial changes even in the active section of the core (irradiation rigs, beam tubes etc), making it impractical, or even impossible to fully capture everything in axially homogeneous slices. In this case, one has to use broader considerations than pure structural variation when placing cuts. The most important factor is to separate regions were large variations in average cross sections are expected, e.g. moving from a highly scattering to a highly absorbing region.

The returned variable cut contains a copy of all the homogenization parameters, and can be used to modify the model, or any other generator parameter for that cut. These are described below.

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Unlike normal active cuts, which tries to mimic two dimensional sections, reflector cuts uses the entire core as a driver region, and contains no axial boundary conditions. Thus, the amount of axial heterogeneity within the section is not an important factor.

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Currently, homogenization calculations are performed on two dimensional slices, or cuts, through the three dimensional heterogeneous model. These cuts are used as building blocks for the homogeneous three dimensional model.

Returns a reference to the underlying heterogeneous model. This can be used to modify the model’s state, change bank positions etc.

Cuts are defined after all the Homogenization Parameters have been set. Standard cuts, which includes source materials, are added using the following function:

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Returns the generator parameter set for the cut. This can be used to modify application parameters, like particles or max_iteration, from the defaults defined in the generator section. These modifications only affect to the current cut.

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