From 4da8d15f58b595f9a2fdedb3f7ca2130eac4a3e6 Mon Sep 17 00:00:00 2001 From: hanemile Date: Mon, 4 Dec 2017 22:34:36 +0100 Subject: updated langfassung --- langfassung/docs/3_hauptteil.tex | 49 ++++++++++++++++++++++++++++++++++++++-- 1 file changed, 47 insertions(+), 2 deletions(-) (limited to 'langfassung/docs/3_hauptteil.tex') diff --git a/langfassung/docs/3_hauptteil.tex b/langfassung/docs/3_hauptteil.tex index eab3897..5174f08 100644 --- a/langfassung/docs/3_hauptteil.tex +++ b/langfassung/docs/3_hauptteil.tex @@ -43,14 +43,59 @@ Blender is Awesome, Python is Awesome and together they are \subsection{Making things faster} -Kicking out to many Stars, 1 out of 10000 is just to much... +\paragraph{ Kicking out to many Stars, 1 out of 10000 is just to much... } +~\\ + +\begin{itemize} + \item Use a custom Density function for each Axis + \begin{itemize} + \item \( \phi(r_x)\), \( \phi(r_y) \) and \( \phi(r_z) \) + \item more controll + \end{itemize} +\end{itemize} + +\begin{tikzpicture} +\begin{scope} + + \node[draw] (H) at (0,-2) + {\( \phi(x_1) > rand_x \)}; + \node[draw] (I) at (5,-2) + {\( \phi(y_1) > rand_y \)}; + \node[draw] (J) at (10,-2) + {\( \phi(z_1) > rand_z \)}; + + \node[draw] (K) at (10, -4) {true}; + \node[draw] (L) at (0, -4) {false}; + + \node[draw] (M) at (10, -6) {write data to data.csv}; + + \node[draw] (N) at (0, -6) {generate new random coordinates}; + +\end{scope} + +\begin{scope} [every node/.style={fill=white,circle}, + every edge/.style={draw=red,very thick}] + + \path[->] (H) edge (K); + \path[->] (I) edge (K); + \path[->] (J) edge (K); + \path[->] (H) edge (L); + \path[->] (I) edge (L); + \path[->] (J) edge (L); + + \path[->] (K) edge (M); + \path[->] (L) edge (N); + +\end{scope} + +\end{tikzpicture} \subsection{Spiral Galaxies} The previous Galaxy models where all using a completely spherical model, generating a spiral galaxy is just not possible using these models. -\subsubsection{N-Körper problem} +\subsubsection{N-body problem} Kurze Beschreibung des N-Körper Problems -- cgit 1.4.1