diff options
| author | Alain Hebert <alainhebert@Alains-MacBook-Pro.local> | 2025-11-02 13:21:20 +0100 |
|---|---|---|
| committer | Alain Hebert <alainhebert@Alains-MacBook-Pro.local> | 2025-11-02 13:21:20 +0100 |
| commit | c234e0ad4a63b37eeb4f93ac05588403a60f2b20 (patch) | |
| tree | 2c6cbaa77460b43053edfb9d865fd568ba160322 /doc/IGE335/Section3.09.tex | |
| parent | bb19a602772d4fe89f5fa2e534b93237330fd89f (diff) | |
#10: Correct a power normalization issue in module EVO:
Diffstat (limited to 'doc/IGE335/Section3.09.tex')
| -rw-r--r-- | doc/IGE335/Section3.09.tex | 3 |
1 files changed, 2 insertions, 1 deletions
diff --git a/doc/IGE335/Section3.09.tex b/doc/IGE335/Section3.09.tex index 1c74f3b..a19d348 100644 --- a/doc/IGE335/Section3.09.tex +++ b/doc/IGE335/Section3.09.tex @@ -409,7 +409,8 @@ fission for fissile nuclide $i$ is calculated as $$E_{{\rm fiss},i}={Q_i \over Q_{\rm 235}} H_{\rm 235}$$ \noindent where $Q_i$ is the fission pseudo-Q value for fissile nuclide $i$; $Q_{\rm 235}$ is the fission pseudo-Q value for U235 and $H_{\rm 235} = 202.27$ MeV is an estimate for the energy deposition per -fission (including the additional energy released in capture reactions) in a typical light water reactor. +fission (including the additional energy released in capture reactions) in a typical light water reactor. This option +assumes that {\tt H-FACTOR} is defined for all heavy isotopes. \item[\moc{NOGL}] keyword to compute the burnup using the energy released by all isotopes present in fuel only. This is the default option. |