Commit 560e8ee6 authored by snuverink_j's avatar snuverink_j
Browse files

small table fix

parent b216a7be
......@@ -320,7 +320,7 @@ See Table~\ref{fieldsolvercmd} for a summary of the Fieldsolver command.
\begin{center}
\caption{Fieldsolver command summary}
\label{tab:fieldsolvercmd}
\begin{tabular}{|l|p{0.6\textwidth}|l|}
\begin{tabular}{|l|l|}
\hline
\tabhead Command & Purpose \\
\hline
......@@ -440,7 +440,7 @@ The behavior of the preconditioner can be: \texttt{STD}\index{PRECMODE!STD}, \te
Suppose $\mathrm{d} E$ the energy spread in the particle bunch is to large, the electrostatic approximation is no longer valid.
One solution to that problem is to introduce $k$ energy bins and perform $k$ separate field solves
in which $\mathrm{d} E$ is again small and hence the electrostatic approximation valid. In case of a cyclotron
see~Section~\ref{cyclotron} the number of energy bins must be at minimum the number of neighboring bunches (\texttt{NNEIGHBB}) i.e. $\text{\texttt{ENBINS}} \le \text{\texttt{NNEIGHBB}}$.
see~Section~\ref{cyclotron} the number of energy bins must be at minimum the number of neighboring bunches (\texttt{NNEIGHBB}) i.e. $\mathrm{ENBINS} \le mathrm{NNEIGHBB}$.
The variable \texttt{MINSTEPFORREBIN} defines the number of integration step that have to pass until all energy bins are merged into one.
......@@ -460,7 +460,7 @@ simulation one requires following ingredients:
\begin{table}[ht] \footnotesize
\begin{center}
\caption{Mesh-refinement strategies}
\caption{Mesh refinement strategies}
\label{tab:tagging_strategies}
\begin{tabular}{|l|p{0.6\textwidth}|}
\hline
......@@ -470,16 +470,16 @@ simulation one requires following ingredients:
scaling factor \texttt{AMR\_SCALING} \\
\texttt{EFIELD} & Mark each cell if the electric field component of any direction satisfies
$E^{level}_{d, cell}\ge\alpha\max E_{d}^{level}$, where $d=x, y, z$ and $\alpha\in[0, 1]$ is the scaling factor
\texttt{AMR\_SCALING} \\
\texttt{AMR\_SCALING} & \\
\texttt{MOMENTA} & It performs a loop over all particles of a level and computes the dot product of the momenta.\ Every
cell that contains a particle with $||\mathbf{p}|| \ge \alpha \max_{level} ||\mathbf{p}||$ is refined.\ The scalar $\alpha\in[0, 1]$
is a user-defined value \texttt{AMR\_SCALING}. \\
\texttt{CHARGE\_DENSITY} & If the charge density of a cell is greater or equal to the value specified with
\texttt{AMD\_DENSITY} the cell is tagged for refinement\\
\texttt{MIN\_NUM\_PARTICLES} & Cells with equal or more particles are refined.\ The bound is specified with
\texttt{AMR\_MIN\_NUM\_PART} \\
\texttt{AMR\_MIN\_NUM\_PART} & \\
\texttt{MAX\_NUM\_PARTICLES} & Cells with equal or less particles are refined.\ The bound is specified with
\texttt{AMR\_MAX\_NUM\_PART}\\
\texttt{AMR\_MAX\_NUM\_PART} & \\
\hline
\end{tabular}
\end{center}
......
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