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Ignore:
Timestamp:
Jul 11, 2005, 6:18:56 PM (21 years ago)
Author:
eugene
Message:

finalize ADD for release (v.12)

File:
1 edited

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  • trunk/doc/pslib/psLibADD.tex

    r4531 r4537  
    1 %%% $Id: psLibADD.tex,v 1.84 2005-07-11 19:36:18 eugene Exp $
     1%%% $Id: psLibADD.tex,v 1.85 2005-07-12 04:18:56 eugene Exp $
    22\documentclass[panstarrs]{panstarrs}
    33
     
    1414\project{Pan-STARRS Image Processing Pipeline}
    1515\organization{Institute for Astronomy}
    16 \version{11}
     16\version{12}
    1717\docnumber{PSDC-430-006}
    1818
     
    23542354The acceleration at the observatory is
    23552355\begin{equation}
    2356  g_1(r_h,\phi) = g(\phi)\left[ 1 - 2( 1 + f + m_r - 2 f {\rm sin}^2\phi)
    2357                    \left(r_h \over a \right) +
    2358                    3 \left(r_h \over a \right)^2 \right]
     2356 g_1(r_h,\phi) = g(\phi)\left[ 1 - 2( 1 + f + m_r - 2 f \sin^2\phi)
     2357                 \left(\frac{r_h}{a} \right) +
     2358               3 \left(\frac{r_h}{a} \right)^2 \right]
    23592359\end{equation}
    23602360where
    23612361\begin{equation}
    2362  g(\phi) = g_e \left( { {1 + k_s {\rm sin}^2 \phi}\over
    2363             \sqrt{1 - \epsilon^2 {\rm sin}^2 \phi}} \right)
     2362 g(\phi) = g_e \left( \frac{1 + k_s \sin^2 \phi}{\sqrt{1 - \epsilon^2 \sin^2 \phi}} \right)
    23642363\end{equation}
    23652364and $\phi$ is the latitude of the observatory and the other constants
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