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lines changed Original file line number Diff line number Diff line change @@ -319,16 +319,18 @@ normalizing reaction rates:
319319
320320 .. math ::
321321
322- \phi = \frac {P}{V \cdot \ sum\limits _i (Q_i \cdot \ sigma ^f_i \cdot n_i)}
322+ \phi = \frac {P}{\ sum\limits _i (Q_i \sigma ^f_i n_i)}
323323
324- where :math: `\sum _i` is the sum over all nuclides :math: `i`. This equation
325- makes the same assumptions and issues as discussed in
326- :ref: `energy-deposition `. Unfortunately, the proposed solution in that
324+ where :math: `P` is the power, :math: `Q_i` is the fission Q value for nuclide
325+ :math: `i`, :math: `\sigma _i^f` is the microscopic fission cross section for
326+ nuclide :math: `i`, and :math: `N_i` is the number of atoms of nuclide
327+ :math: `i`. This equation makes the same assumptions and issues as discussed
328+ in :ref: `energy-deposition `. Unfortunately, the proposed solution in that
327329 section does not apply here since we are decoupled from transport code.
328330 However, there is a method to converge to a more accurate value for flux by
329- using substeps during time integration.
330- ` This paper <https://doi.org/10.1016/j.anucene.2016.05.031 >`_ provides a
331- good discussion of this method.
331+ using substeps during time integration. ` This paper
332+ <https://doi.org/10.1016/j.anucene.2016.05.031> `_ provides a good discussion
333+ of this method.
332334
333335.. warning ::
334336
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