[cig-commits] [commit] devel: doc: Use AMS's align instead of eqnarray. (c11f41c)

[cig_noreply at geodynamics.org]

Repository : ssh://geoshell/specfem2d

On branch  : devel
Link       : https://github.com/geodynamics/specfem2d/compare/24dca31bf087ee51d2d1db912640d58ade2df07c...a3880316a04510a6c88ed36ceee2fab3c0169f6e

>---------------------------------------------------------------

commit c11f41cb177758efe09e3dafc9adb5b2b0914cf2
Author: Elliott Sales de Andrade <esalesde at physics.utoronto.ca>
Date:   Mon Jan 27 18:11:19 2014 -0500

    doc: Use AMS's align instead of eqnarray.
    
    This is the recommended environment due to spacing differences between
    eqnarray and normal equations.


>---------------------------------------------------------------

c11f41cb177758efe09e3dafc9adb5b2b0914cf2
 doc/USER_MANUAL/manual_SPECFEM2D.pdf | Bin 3119917 -> 3127219 bytes
 doc/USER_MANUAL/manual_SPECFEM2D.tex |  18 +++++++++---------
 2 files changed, 9 insertions(+), 9 deletions(-)

diff --git a/doc/USER_MANUAL/manual_SPECFEM2D.pdf b/doc/USER_MANUAL/manual_SPECFEM2D.pdf
index deb1ccd..f288828 100644
Binary files a/doc/USER_MANUAL/manual_SPECFEM2D.pdf and b/doc/USER_MANUAL/manual_SPECFEM2D.pdf differ
diff --git a/doc/USER_MANUAL/manual_SPECFEM2D.tex b/doc/USER_MANUAL/manual_SPECFEM2D.tex
index a0b66f5..8407114 100644
--- a/doc/USER_MANUAL/manual_SPECFEM2D.tex
+++ b/doc/USER_MANUAL/manual_SPECFEM2D.tex
@@ -82,7 +82,7 @@
 \title{\textbf{SPECFEM2D}\\
 \textbf{User Manual}}
 
-\author{$\copyright$ Princeton University (USA) and CNRS and University of Marseille (France)\\
+\author{\copyright\ Princeton University (USA) and CNRS and University of Marseille (France)\\
 Version 7.0
 }
 
@@ -1226,13 +1226,13 @@ We also changed the relationship between adjoint potential and adjoint displacem
 The new definition is critical when there are adjoint sources (in other words, receivers) in the acoustic domain,
 and is the direct consequence of the optimization problem.
 %
-\begin{eqnarray*}
-\mathbf{s}&\equiv&\frac{1}{\rho}~\mathbf{\nabla}\phi \\
-p&\equiv&-\kappa(\nabla\cdot\mathbf{s}) =-\partial_t^2\phi \\
-\quad\\
-\partial_t^2\mathbf{s}^\dagger&\equiv&-\frac{1}{\rho}~\mathbf{\nabla}\phi^\dagger\\
-p^\dagger&\equiv&-\kappa(\nabla\cdot\mathbf{s}^\dagger)=\phi^\dagger
-\end{eqnarray*}
+\begin{align*}
+\mathbf{s} &\equiv \frac{1}{\rho} \: \mathbf{\nabla}\phi \\
+p &\equiv -\kappa\left(\nabla\cdot\mathbf{s}\right) = -\partial_t^2\phi \\
+&\\
+\partial_t^2\mathbf{s}^\dagger &\equiv -\frac{1}{\rho} \: \mathbf{\nabla}\phi^\dagger \\
+p^\dagger &\equiv -\kappa\left(\nabla\cdot\mathbf{s}^\dagger\right) = \phi^\dagger
+\end{align*}
 
 
 
@@ -1264,7 +1264,7 @@ Main historical authors: Dimitri Komatitsch and Jeroen Tromp
 Princeton University, USA,
 and CNRS / INRIA / University of Pau, France
 
-$\copyright$ Princeton University and CNRS / INRIA / University of Pau, July 2012
+\copyright\ Princeton University and CNRS / INRIA / University of Pau, July 2012
 \end{quote}
 
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