Changeset 11558 for NEMO/trunk/doc/latex/NEMO/subfiles/apdx_s_coord.tex

Timestamp:

2019-09-17T17:04:06+02:00 (5 years ago)

Author:

nicolasmartin

Message:

Review all figure envs + activation of listoflistings

1. Figure env:
   • Replace center sub-env with only \centering cmd
   • Add alternate caption for \listoffigures (shorter one between square brackets, i.e. \caption[]{})
   • Place \label outside of \caption and remove useless \protect

2. Namelist listings
   • Put \nlst with the namelist inlcusion in a listing float env with caption and label
   • Remove namelist duplicates

-- This line, and those below, will be ignored--
M subfiles/apdx_triads.tex
M subfiles/chap_model_basics_zstar.tex
M subfiles/chap_SBC.tex
M subfiles/apdx_DOMAINcfg.tex
M subfiles/apdx_s_coord.tex
M subfiles/chap_DOM.tex
M subfiles/chap_ASM.tex
M subfiles/chap_DIU.tex
M subfiles/chap_cfgs.tex
M subfiles/chap_ZDF.tex
M subfiles/chap_OBS.tex
M subfiles/chap_model_basics.tex
M subfiles/chap_time_domain.tex
M subfiles/apdx_algos.tex
M subfiles/chap_TRA.tex
M subfiles/chap_DYN.tex
M subfiles/chap_misc.tex
M subfiles/chap_DIA.tex
M subfiles/apdx_invariants.tex
M subfiles/chap_LBC.tex
M subfiles/apdx_diff_opers.tex
M subfiles/chap_STO.tex
M subfiles/chap_LDF.tex

File:

• NEMO/trunk/doc/latex/NEMO/subfiles/apdx_s_coord.tex (modified) (5 diffs)

NEMO/trunk/doc/latex/NEMO/subfiles/apdx_s_coord.tex

@@ -63 +63 @@
 Using the first form and considering a change $\delta i$ with $j, z$ and $t$ held constant, shows that
 \begin{equation}
-  \label{eq:SCOORD_s_chain_rule}
+  \label{eq:SCOORD_s_chain_rule1}
       \left. {\frac{\partial \bullet }{\partial i}} \right|_{j,z,t}  =
       \left. {\frac{\partial \bullet }{\partial i}} \right|_{j,s,t}
@@ -102 +102 @@
 the model equations in the curvilinear $s-$coordinate system are:
 \begin{equation}
-  \label{eq:SCOORD_s_chain_rule}
+  \label{eq:SCOORD_s_chain_rule2}
   \begin{aligned}
     &\left. {\frac{\partial \bullet }{\partial t}} \right|_z  =
@@ -128 +128 @@
 \label{sec:SCOORD_continuity}
 
-Using (\autoref{eq:SCOORD_s_chain_rule}) and
+Using (\autoref{eq:SCOORD_s_chain_rule1}) and
 the fact that the horizontal scale factors $e_1$ and $e_2$ do not depend on the vertical coordinate,
 the divergence of the velocity relative to the ($i$,$j$,$z$) coordinate system is transformed as follows in order to
@@ -272 +272 @@
         +  w \;\frac{\partial u}{\partial z}      \\
         %
-      \intertext{introducing the chain rule (\autoref{eq:SCOORD_s_chain_rule}) }
+      \intertext{introducing the chain rule (\autoref{eq:SCOORD_s_chain_rule1}) }
       %
       &= \left. {\frac{\partial u }{\partial t}} \right|_z
@@ -317 +317 @@
 \end{subequations}
 %
-Applying the time derivative chain rule (first equation of (\autoref{eq:SCOORD_s_chain_rule})) to $u$ and
+Applying the time derivative chain rule (first equation of (\autoref{eq:SCOORD_s_chain_rule1})) to $u$ and
 using (\autoref{eq:SCOORD_w_in_s}) provides the expression of the last term of the right hand side,
 \[