From c234e0ad4a63b37eeb4f93ac05588403a60f2b20 Mon Sep 17 00:00:00 2001
From: Alain Hebert <alainhebert@Alains-MacBook-Pro.local>
Date: Sun, 2 Nov 2025 13:21:20 +0100
Subject: #10: Correct a power normalization issue in module EVO:

---
 doc/IGE335/Section3.09.tex | 3 ++-
 1 file changed, 2 insertions(+), 1 deletion(-)

(limited to 'doc/IGE335/Section3.09.tex')

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.
-- 
cgit v1.2.3

