| 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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