X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/book_gpu.git/blobdiff_plain/553cf9105cef21498f722907ddff0a480b77d6b2..177d75ae3d1a1061fb9caa43de9afca760ca0d1a:/BookGPU/Chapters/chapter14/ch14.tex?ds=inline

diff --git a/BookGPU/Chapters/chapter14/ch14.tex b/BookGPU/Chapters/chapter14/ch14.tex
index 9759ba7..d50db31 100755
--- a/BookGPU/Chapters/chapter14/ch14.tex
+++ b/BookGPU/Chapters/chapter14/ch14.tex
@@ -7,7 +7,7 @@ application}
 
 
 \section{Introduction}
-The lattice Boltzmann (LB) method (for an overview see, e.g.,
+The lattice Boltzmann (LB) method \index{Lattice Boltzmann method} (for an overview see, e.g.,
 \cite{succi-book}) has become a popular approach to a variety of fluid
 dynamics problems.  It provides a way to solve the incompressible,
 isothermal Navier-Stokes equations and has the attractive features of
@@ -55,7 +55,7 @@ and particle suspensions, and typically require additional physics
 beyond the bare Navier-Stokes equations to provide a full
 description~\cite{aidun2010}. The representation of this extra
 physics raises additional design questions for the application
-programmer. Here, we consider the \textit{Ludwig} code \cite{desplat},
+programmer. Here, we consider the \textit{Ludwig} code \cite{desplat}\index{Ludwig code},
 an LB application developed specifically for complex fluids
 (\textit{Ludwig} was named for Boltzmann, 1844--1906).
 We will present the steps