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1 % $Header: /u/u0/gcmpack/mitgcmdoc/part1/appendix_operators.tex,v 1.2 2001/09/27 01:57:17 cnh Exp $
2 % $Name: $
3
4 \section{Appendix:OPERATORS}
5
6 \subsection{Coordinate systems}
7
8 \subsubsection{Spherical coordinates}
9
10 In spherical coordinates, the velocity components in the zonal, meridional
11 and vertical direction respectively, are given by (see Fig.2) :
12
13 \[
14 u=r\cos \phi \frac{D\lambda }{Dt}
15 \]
16
17 \[
18 v=r\frac{D\phi }{Dt}\qquad
19 \]
20 $\qquad \qquad \qquad \qquad $
21
22 \[
23 \dot{r}=\frac{Dr}{Dt}
24 \]
25
26 Here $\phi $ is the latitude, $\lambda $ the longitude, $r$ the radial
27 distance of the particle from the center of the earth, $\Omega $ is the
28 angular speed of rotation of the Earth and $D/Dt$ is the total derivative.
29
30 Fig.2. The spherical polar velocities $(u,v,\dot{r})$, the latitude is $\phi
31 $ and the longitude $\lambda $.
32
33 The `grad' ($\nabla $) and `div' ($\nabla $.) operators are defined by, in
34 spherical coordinates:
35
36 \[
37 \nabla \equiv \left( \frac{1}{r\cos \phi }\frac{\partial }{\partial \lambda }
38 ,\frac{1}{r}\frac{\partial }{\partial \phi },\frac{\partial }{\partial r}
39 \right)
40 \]
41
42 \[
43 \nabla .v\equiv \frac{1}{r\cos \phi }\left\{ \frac{\partial u}{\partial
44 \lambda }+\frac{\partial }{\partial \phi }\left( v\cos \phi \right) \right\}
45 +\frac{1}{r^{2}}\frac{\partial \left( r^{2}\dot{r}\right) }{\partial r}
46 \]

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