X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/book_gpu.git/blobdiff_plain/4932967a1c684dc3f7ed04c19144101278b79972..HEAD:/BookGPU/Chapters/chapter16/intro.tex?ds=inline

diff --git a/BookGPU/Chapters/chapter16/intro.tex b/BookGPU/Chapters/chapter16/intro.tex
index cbed054..6d021c3 100644
--- a/BookGPU/Chapters/chapter16/intro.tex
+++ b/BookGPU/Chapters/chapter16/intro.tex
@@ -11,7 +11,7 @@ switching power converters. The new method first exploits the
 parallelisim in the envelope-following method and parallelize the
 Newton update solving part, which is the most computational expensive,
 in GPU platforms to boost the simulation performance.  To further
-speed up the iterative GMRES\index{GMRES} solving for Newton update equation in the
+speed up the iterative GMRES\index{iterative method!GMRES} solving for Newton update equation in the
 envelope-following method, we apply the matrix-free\index{matrix-free}
 Krylov subspace\index{Krylov subspace} basis
 generation technique, which was previously used for RF simulation.
@@ -42,7 +42,7 @@ In those switching power converters, it is the envelope,
 which is the power voltage delivered,
 not the fast switching waves in every cycle,
 that is of interest to the designers.
-As shown in Fig.~\ref{fig:ef1}, the solid line is
+As shown in Figure~\ref{fig:ef1}, the solid line is
 the waveform of the output node in a Buck
 converter~\cite{Krein:book'97}, the dots are the simulation points
 of SPICE\index{SPICE}, and the appended dash line is the envelope.
@@ -54,7 +54,7 @@ clock cycle to get the accurate details of the carrier.  For
 switching power converters, the waveform of the carrier in
 consequent cycles does not change much, envelope-following method
 is an approximation analysis method, which skips over several
-cycles (the dash line in Fig.~\ref{fig:ef2}), the so called
+cycles (the dash line in Figure~\ref{fig:ef2}), the so called
 envelope step, without simulating them, and then carries out a
 correction, which usually contains a sensitivity-based Newton
 iteration or shooting until convergence, in order to begin the
@@ -75,14 +75,14 @@ next envelope step.
   \subfigure[The envelope changes in a slow time scale.]
        {\resizebox{.9\textwidth}{!}{\input{./Chapters/chapter16/figures/envelope.pdf_t}}
             \label{fig:ef2} }
-  \caption{Transient envelope-following\index{envelope-following} analysis.
-    (Both two figures reflect backward-Euler\index{backward-Euler} style envelope-following.)}
+  \caption[Transient envelope-following\index{envelope-following} analysis.]{Transient envelope-following\index{envelope-following} analysis.
+    (Both figures reflect backward Euler\index{Euler!backward Euler} style envelope-following.)}
   \label{fig:ef_intro}
 \end{figure}
 
 %\IEEEpubidadjcol
 
-Also, iterative GMRES\index{GMRES} solver is typically used in the
+Also, iterative GMRES\index{iterative method!GMRES} solver is typically used in the
 envelope-following method to compute the solution of Newton update
 due to its efficiency compared to direct LU\index{LU} method.
 However, as the Jacobian matrix\index{Jacobian matrix}
