\chapter{Concepts}\index{Concepts}%
\setheader{{\it CHAPTER \thechapter}}{}{}{}{}{{\it CHAPTER \thechapter}}%
-\setfooter{\thepage}{}{}{}{\small Manual v0.2}{\thepage}%
+\ctsimfooter%
\section{Overview}\label{conceptoverview}\index{Concepts,Overview}%
The operation of \ctsim\ begins with the phantom object. A
For parallel geometry scanning, the focal length doesn't matter.
However, divergent geometry scanning (equilinear and equiangular),
the \emph{focal length ratio} should be set at \texttt{2} or more
-to avoid artifacts. Moreover, a value of less than \texttt{1},
-though it can be given to \ctsim, is physically impossible and it
-analagous to have having the x-ray source with the \emph{view
-diameter}.
+to avoid artifacts. Moreover, a value of less than \texttt{1} is
+physically impossible and it analagous to have having the x-ray
+source inside of the \emph{view diameter}.
\subsection{Parallel Geometry}\label{geometryparallel}\index{Concepts,Scanner,Geometries,Parallel}
covering an angular distance of
\latexonly{$2\,\alpha$.}\latexignore{\emph{2 \alpha}.} The dotted
circle in
-\begin{figure}
-\image{10cm;0cm}{equiangular.eps}
-\caption{Equiangluar geometry}
+\begin{figure}\label{equiangularfig}
+\image{10cm;0cm}{equiangular.eps} \caption{Equiangular geometry}
\end{figure}
figure 2.4 indicates the positions of the detectors in this case.
\latexonly{$\alpha$}\latexignore{\emph{alpha}} and the \emph{focal
length}. It is calculated as \latexonly{$4\,f \tan (\alpha / 2)$}
\latexignore{\emph{4 x F x tan(\alpha/2)}}
-\begin{figure}
+\begin{figure}\label{equilinearfig}
\image{10cm;0cm}{equilinear.eps}
\caption{Equilinear geometry}
\end{figure}
-An example of the this geometry is in figure 2.5.
+This geometry is shown in figure~2.5.
\subsubsection{Examples of Geometry Settings}