27 |
\end{equation} |
\end{equation} |

28 |
where $\gamma$ is the gravitational constant. |
where $\gamma$ is the gravitational constant. |

29 |
Consider now the \esc general form, which can simply be related to |
Consider now the \esc general form, which can simply be related to |

30 |
\auoref{eqn:poisson} using two coefficients. The result is |
\autoref{eqn:poisson} using two coefficients. The result is |

31 |
\begin{equation} |
\begin{equation} |

32 |
-\left(A\hackscore{jl} u\hackscore{,l} \right)\hackscore{,j} = Y |
-\left(A\hackscore{jl} u\hackscore{,l} \right)\hackscore{,j} = Y |

33 |
\end{equation} |
\end{equation} |