Changeset 4530 for trunk/doc/pslib/psLibADD.tex
- Timestamp:
- Jul 11, 2005, 9:17:38 AM (21 years ago)
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trunk/doc/pslib/psLibADD.tex (modified) (11 diffs)
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trunk/doc/pslib/psLibADD.tex
r4529 r4530 1 %%% $Id: psLibADD.tex,v 1.8 2 2005-07-09 02:25:56eugene Exp $1 %%% $Id: psLibADD.tex,v 1.83 2005-07-11 19:17:38 eugene Exp $ 2 2 \documentclass[panstarrs]{panstarrs} 3 3 … … 1811 1811 is broken down into a number of steps as described below. 1812 1812 1813 \ paragraph{Reference Implementations}1814 1815 There are two reference implementati ns for the code to account for the1813 \subsubsection{Reference Implementations} 1814 1815 There are two reference implementations for the code to account for the 1816 1816 motion of the Earth in space. The first are the sample routines 1817 1817 provided by the IERS to accompany chaper 5 of IERS Bulletin … … 2234 2234 2235 2235 \paragraph{Atmospheric Refraction} 2236 \newcommand\citep[1]{\textit{#1}} 2237 \newcommand\citet[1]{\textit{#1}} 2236 2238 2237 2239 {\em The following discussion is adapted from an article by Ken Chambers} 2238 \newcommand\citep{\em}2239 \newcommand\citet{\em}2240 2240 2241 2241 The hypsometric structure and index of refraction of the Earth's … … 2313 2313 divided into separate subsections. 2314 2314 2315 \sub section{Observatory height}2315 \subparagraph{Observatory height} 2316 2316 2317 2317 The height of the observatory from the geometric center … … 2330 2330 (i.e. a local plumb line). 2331 2331 2332 \sub section{The magnitude of normal gravity at the observatory }2332 \subparagraph{The magnitude of normal gravity at the observatory } 2333 2333 2334 2334 The local magnitude of normal gravity … … 2391 2391 2392 2392 2393 \sub section{The scale height above the observatory}2393 \subparagraph{The scale height above the observatory} 2394 2394 2395 2395 The scale height of the atmosphere above the observatory is … … 2496 2496 \end{equation} 2497 2497 2498 \sub section{The index of refraction of moist air at the observatory}2498 \subparagraph{The index of refraction of moist air at the observatory} 2499 2499 2500 2500 The Ciddor equation for the index of refraction of moist air … … 2594 2594 \end{table} 2595 2595 2596 2597 \subsection{The tropopause term in the equation of refraction} 2596 \subparagraph{The tropopause term in the equation of refraction} 2598 2597 2599 2598 The final term in the Refraction Equation (2) … … 2625 2624 \end{equation} 2626 2625 2627 \sub section{Calculating the atmospheric refraction from both2628 the observed and true zenith angle}2626 \subparagraph{Calculating the atmospheric refraction from both 2627 the observed and true zenith angle} 2629 2628 2630 2629 The monochromatic refraction can now be calculated for any given wavelength … … 2671 2670 \end{equation} 2672 2671 2673 \section{Atmospheric Dispersion} 2674 2675 The atmospheric dispersion is then 2676 \begin{equation} 2677 { \overline{(R- \bar R)^2}} = {{\int (R - \bar R)^2 N_{\lambda} d \lambda} \over 2678 {\int N_{\lambda} d\lambda}} 2679 \end{equation} 2680 2681 \section{Air Mass and Extinction} 2672 \subsubsection{Air Mass and Extinction} 2682 2673 2683 2674 By Laplace's theorem, the monochromatic airmass (mass per unit area … … 2715 2706 accurate expression for airmass should lead to improved extinction 2716 2707 corrections at high airmass. 2717 2718 \section{Limits to ground based relative and absolute astrometry}2719 2720 The limits to ground based astrometry may well be our abilitiy to2721 measure the atmospheric profile along the line of sight of a given2722 observation, and the systematic limit of the telescope axes encoders2723 (and sophistication of the telescope mount model.)2724 The refratction model above requires only the additional data of2725 the temperature, height, and presure of the tropopause, but much more2726 detailed atmospheric information will be available for PS1 from our sky2727 probes which measure atmospheric absorption for each field and even,2728 phase drifts of GPS clocks from Rubidium or Cesium standard clocks.2729 These can be converted directly into a nearby line of sight index of refraction2730 at optical wavelengths. Thus we encourage wide field survey telescopes to2731 err on the side of over instrumenting the accuracy and repeatibility2732 of the axes encoders.2733 2734 2735 2708 2736 2709 \subsection{Projections}
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