From 9983cfc21ccdc89337abe2f5c331bf9e21d93efa Mon Sep 17 00:00:00 2001
From: Stefania Ciliberti <stefania.ciliberti@cmcc.it>
Date: Sun, 27 Feb 2022 08:05:35 +0100
Subject: [PATCH] revised text for dynspg_exp and dynspg_ts
---
doc/latex/NEMO/subfiles/chap_DYN.tex | 8 ++++----
1 file changed, 4 insertions(+), 4 deletions(-)
diff --git a/doc/latex/NEMO/subfiles/chap_DYN.tex b/doc/latex/NEMO/subfiles/chap_DYN.tex
index f61cdb29..0aa8a474 100644
--- a/doc/latex/NEMO/subfiles/chap_DYN.tex
+++ b/doc/latex/NEMO/subfiles/chap_DYN.tex
@@ -793,11 +793,11 @@ so that the update of the next velocities is done in module \mdl{dynspg\_flt} an
The form of the surface pressure gradient term depends on how the user wants to
handle the fast external gravity waves that are a solution of the analytical equation (\autoref{sec:MB_hor_pg}).
-Three formulations are available, all controlled by a CPP key (ln\_dynspg\_xxx):
+Two formulations are available, all controlled by a CPP key (ln\_dynspg\_<method>):
an explicit formulation which requires a small time step;
-a filtered free surface formulation which allows a larger time step by
-adding a filtering term into the momentum equation;
-and a split-explicit free surface formulation, described below, which also allows a larger time step.
+%a filtered free surface formulation which allows a larger time step by
+%adding a filtering term into the momentum equation;
+a split-explicit free surface formulation which also allows a larger time step.
The extra term introduced in the filtered method is calculated implicitly, so that a solver is used to compute it.
As a consequence the update of the $next$ velocities is done in module \mdl{dynspg\_flt} and not in \mdl{dynnxt}.
--
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