| 1 | /* | 
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| 2 | *+ | 
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| 3 | *  Name: | 
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| 4 | *     palRefz | 
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| 5 |  | 
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| 6 | *  Purpose: | 
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| 7 | *     Adjust unrefracted zenith distance | 
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| 8 |  | 
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| 9 | *  Language: | 
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| 10 | *     Starlink ANSI C | 
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| 11 |  | 
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| 12 | *  Type of Module: | 
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| 13 | *     Library routine | 
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| 14 |  | 
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| 15 | *  Invocation: | 
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| 16 | *     void palRefz ( double zu, double refa, double refb, double *zr ); | 
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| 17 |  | 
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| 18 | *  Arguments: | 
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| 19 | *     zu = double (Given) | 
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| 20 | *         Unrefracted zenith distance of the source (radians) | 
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| 21 | *     refa = double (Given) | 
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| 22 | *         tan Z coefficient (radians) | 
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| 23 | *     refb = double (Given) | 
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| 24 | *         tan**3 Z coefficient (radian) | 
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| 25 | *     zr = double * (Returned) | 
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| 26 | *         Refracted zenith distance (radians) | 
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| 27 |  | 
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| 28 | *  Description: | 
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| 29 | *     Adjust an unrefracted zenith distance to include the effect of | 
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| 30 | *     atmospheric refraction, using the simple A tan Z + B tan**3 Z | 
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| 31 | *     model (plus special handling for large ZDs). | 
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| 32 |  | 
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| 33 | *  Authors: | 
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| 34 | *     PTW: Patrick T. Wallace | 
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| 35 | *     TIMJ: Tim Jenness (JAC, Hawaii) | 
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| 36 | *     {enter_new_authors_here} | 
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| 37 |  | 
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| 38 | *  Notes: | 
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| 39 | *     - This routine applies the adjustment for refraction in the | 
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| 40 | *     opposite sense to the usual one - it takes an unrefracted | 
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| 41 | *     (in vacuo) position and produces an observed (refracted) | 
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| 42 | *     position, whereas the A tan Z + B tan**3 Z model strictly | 
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| 43 | *     applies to the case where an observed position is to have the | 
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| 44 | *     refraction removed.  The unrefracted to refracted case is | 
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| 45 | *     harder, and requires an inverted form of the text-book | 
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| 46 | *     refraction models;  the formula used here is based on the | 
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| 47 | *     Newton-Raphson method.  For the utmost numerical consistency | 
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| 48 | *     with the refracted to unrefracted model, two iterations are | 
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| 49 | *     carried out, achieving agreement at the 1D-11 arcseconds level | 
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| 50 | *     for a ZD of 80 degrees.  The inherent accuracy of the model | 
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| 51 | *     is, of course, far worse than this - see the documentation for | 
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| 52 | *     palRefco for more information. | 
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| 53 | * | 
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| 54 | *     - At ZD 83 degrees, the rapidly-worsening A tan Z + B tan^3 Z | 
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| 55 | *     model is abandoned and an empirical formula takes over.  For | 
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| 56 | *     optical/IR wavelengths, over a wide range of observer heights and | 
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| 57 | *     corresponding temperatures and pressures, the following levels of | 
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| 58 | *     accuracy (arcsec, worst case) are achieved, relative to numerical | 
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| 59 | *     integration through a model atmosphere: | 
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| 60 | * | 
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| 61 | *              ZR    error | 
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| 62 | * | 
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| 63 | *              80      0.7 | 
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| 64 | *              81      1.3 | 
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| 65 | *              82      2.4 | 
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| 66 | *              83      4.7 | 
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| 67 | *              84      6.2 | 
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| 68 | *              85      6.4 | 
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| 69 | *              86      8 | 
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| 70 | *              87     10 | 
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| 71 | *              88     15 | 
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| 72 | *              89     30 | 
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| 73 | *              90     60 | 
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| 74 | *              91    150         } relevant only to | 
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| 75 | *              92    400         } high-elevation sites | 
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| 76 | * | 
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| 77 | *     For radio wavelengths the errors are typically 50% larger than | 
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| 78 | *     the optical figures and by ZD 85 deg are twice as bad, worsening | 
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| 79 | *     rapidly below that.  To maintain 1 arcsec accuracy down to ZD=85 | 
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| 80 | *     at the Green Bank site, Condon (2004) has suggested amplifying | 
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| 81 | *     the amount of refraction predicted by palRefz below 10.8 deg | 
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| 82 | *     elevation by the factor (1+0.00195*(10.8-E_t)), where E_t is the | 
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| 83 | *     unrefracted elevation in degrees. | 
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| 84 | * | 
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| 85 | *     The high-ZD model is scaled to match the normal model at the | 
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| 86 | *     transition point;  there is no glitch. | 
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| 87 | * | 
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| 88 | *     - Beyond 93 deg zenith distance, the refraction is held at its | 
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| 89 | *     93 deg value. | 
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| 90 | * | 
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| 91 | *     - See also the routine palRefv, which performs the adjustment in | 
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| 92 | *     Cartesian Az/El coordinates, and with the emphasis on speed | 
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| 93 | *     rather than numerical accuracy. | 
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| 94 |  | 
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| 95 | *  References: | 
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| 96 | *     Condon,J.J., Refraction Corrections for the GBT, PTCS/PN/35.2, | 
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| 97 | *     NRAO Green Bank, 2004. | 
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| 98 |  | 
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| 99 | *  History: | 
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| 100 | *     2012-08-24 (TIMJ): | 
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| 101 | *        Initial version, ported directly from Fortran SLA | 
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| 102 | *        Adapted with permission from the Fortran SLALIB library. | 
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| 103 | *     {enter_further_changes_here} | 
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| 104 |  | 
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| 105 | *  Copyright: | 
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| 106 | *     Copyright (C) 2004 Rutherford Appleton Laboratory | 
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| 107 | *     Copyright (C) 2012 Science and Technology Facilities Council. | 
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| 108 | *     All Rights Reserved. | 
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| 109 |  | 
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| 110 | *  Licence: | 
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| 111 | *     This program is free software; you can redistribute it and/or | 
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| 112 | *     modify it under the terms of the GNU General Public License as | 
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| 113 | *     published by the Free Software Foundation; either version 3 of | 
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| 114 | *     the License, or (at your option) any later version. | 
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| 115 | * | 
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| 116 | *     This program is distributed in the hope that it will be | 
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| 117 | *     useful, but WITHOUT ANY WARRANTY; without even the implied | 
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| 118 | *     warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR | 
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| 119 | *     PURPOSE. See the GNU General Public License for more details. | 
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| 120 | * | 
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| 121 | *     You should have received a copy of the GNU General Public License | 
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| 122 | *     along with this program; if not, write to the Free Software | 
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| 123 | *     Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, | 
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| 124 | *     MA 02110-1301, USA. | 
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| 125 |  | 
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| 126 | *  Bugs: | 
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| 127 | *     {note_any_bugs_here} | 
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| 128 | *- | 
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| 129 | */ | 
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| 130 |  | 
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| 131 | #include <math.h> | 
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| 132 |  | 
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| 133 | #include "pal.h" | 
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| 134 | #include "palmac.h" | 
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| 135 |  | 
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| 136 | void palRefz ( double zu, double refa, double refb, double *zr ) { | 
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| 137 |  | 
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| 138 | /* Constants */ | 
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| 139 |  | 
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| 140 | /* Largest usable ZD (deg) */ | 
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| 141 | const double D93 = 93.0; | 
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| 142 |  | 
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| 143 | /* ZD at which one model hands over to the other (radians) */ | 
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| 144 | const double Z83 = 83.0 * PAL__DD2R; | 
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| 145 |  | 
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| 146 | /* coefficients for high ZD model (used beyond ZD 83 deg) */ | 
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| 147 | const double C1 = +0.55445; | 
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| 148 | const double C2 = -0.01133; | 
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| 149 | const double C3 = +0.00202; | 
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| 150 | const double C4 = +0.28385; | 
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| 151 | const double C5 = +0.02390; | 
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| 152 |  | 
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| 153 | /* High-ZD-model prefiction (deg) for that point */ | 
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| 154 | const double REF83 = (C1+C2*7.0+C3*49.0)/(1.0+C4*7.0+C5*49.0); | 
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| 155 |  | 
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| 156 | double zu1,zl,s,c,t,tsq,tcu,ref,e,e2; | 
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| 157 |  | 
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| 158 | /*  perform calculations for zu or 83 deg, whichever is smaller */ | 
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| 159 | zu1 = DMIN(zu,Z83); | 
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| 160 |  | 
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| 161 | /*  functions of ZD */ | 
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| 162 | zl = zu1; | 
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| 163 | s = sin(zl); | 
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| 164 | c = cos(zl); | 
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| 165 | t = s/c; | 
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| 166 | tsq = t*t; | 
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| 167 | tcu = t*tsq; | 
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| 168 |  | 
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| 169 | /*  refracted zd (mathematically to better than 1 mas at 70 deg) */ | 
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| 170 | zl = zl-(refa*t+refb*tcu)/(1.0+(refa+3.0*refb*tsq)/(c*c)); | 
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| 171 |  | 
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| 172 | /*  further iteration */ | 
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| 173 | s = sin(zl); | 
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| 174 | c = cos(zl); | 
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| 175 | t = s/c; | 
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| 176 | tsq = t*t; | 
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| 177 | tcu = t*tsq; | 
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| 178 | ref = zu1-zl+ | 
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| 179 | (zl-zu1+refa*t+refb*tcu)/(1.0+(refa+3.0*refb*tsq)/(c*c)); | 
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| 180 |  | 
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| 181 | /*  special handling for large zu */ | 
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| 182 | if (zu > zu1) { | 
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| 183 | e = 90.0-DMIN(D93,zu*PAL__DR2D); | 
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| 184 | e2 = e*e; | 
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| 185 | ref = (ref/REF83)*(C1+C2*e+C3*e2)/(1.0+C4*e+C5*e2); | 
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| 186 | } | 
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| 187 |  | 
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| 188 | /*  return refracted zd */ | 
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| 189 | *zr = zu-ref; | 
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| 190 |  | 
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| 191 | } | 
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