diff options
Diffstat (limited to 'doc')
| -rw-r--r-- | doc/IGE335/Section3.09.tex | 3 | ||||
| -rw-r--r-- | doc/IGE351/SectDburnup.tex | 1 |
2 files changed, 3 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. diff --git a/doc/IGE351/SectDburnup.tex b/doc/IGE351/SectDburnup.tex index 07cb0d4..76cac21 100644 --- a/doc/IGE351/SectDburnup.tex +++ b/doc/IGE351/SectDburnup.tex @@ -63,6 +63,7 @@ $I_{g}=\mathcal{S}^{b}_{10}$ where \begin{displaymath} I_{g} = \left\{ \begin{array}{rl} + -1 & \textrm{Compute the burnup using the fission rate in $^{235}U$ multiplied by 202.27 MeV} \\ 0 & \textrm{Compute the burnup using the power released in fuel} \\ 1 & \textrm{Compute the burnup using the power released in the global geometry} \\ \end{array} \right. |