Changes between Version 59 and Version 60 of SelfGravityDevel

Timestamp:

02/05/13 13:20:33 (12 years ago)

Author:

Jonathan

Comment:

Reverted to version 44.

SelfGravityDevel

@@ -28 +28 @@
 #!latex
 \begin{equation}\label{eq:uniDensity}\tag{1}
-\rho= \begin{cases} \rho_0 & r < R \\
-                   0 & r \ge R 
+\rho= \begin{cases} \rho_{0}, &r < R \\
+                   0, & r\ge R 
      \end{cases}
 \end{equation}
 }}}
 
-{{{
-#!latex
-\begin{equation}\label{eq:uniDensity2}\tag{11}
-\rho= \begin{cases} \rho_0 & r < R \\
-0 & r \ge R
-\end{cases}
-\end{equation}
-}}}
-
-
-{{{
-#!latex
-\begin{equation}\label{eq:uniDensity3}\tag{12}
-\rho=\begin{cases} \rho_0 & r < R \\
-0 & r \ge R
-\end{cases}
-\end{equation}
-}}}
-
-{{{
-#!latex
-\begin{equation}\label{eq:uniDensity4}\tag{13}
-\rho=\begin{cases} \rho_0 & r < R \\
-0 & r \ge R
-\end{cases}
-\end{equation}
-}}}
 
  Use spherical coordinates, the Poisson equation for the density distribution Equation (1) can be written as
@@ -84 +57 @@
 #!latex
 \begin{equation}\label{eq:solUniSphere}\tag{4}
-\phi(r)=\begin{cases} -\frac{4 \pi}{3} G\rho \frac{R^{3}}{r} & r>R\\
+\phi(r)=\begin{cases} -\frac{4\pi}{3} G\rho \frac{R^{3}}{r} & r>R\\
          -\frac{2\pi G\rho}{3}\left[R^{2}-r^{2}\right]-\frac{4\pi}{3}G\rho R^{2} &r\ge R
         \end{cases}