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/* |
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*+ |
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* Name: |
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* palAtmdsp |
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* Purpose: |
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* Apply atmospheric-dispersion adjustments to refraction coefficients |
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* Language: |
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* Starlink ANSI C |
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* Type of Module: |
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* Library routine |
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* Invocation: |
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* void palAtmdsp( double tdk, double pmb, double rh, double wl1, |
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* double a1, double b1, double wl2, double *a2, double *b2 ); |
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20
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* Arguments: |
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* tdk = double (Given) |
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* Ambient temperature, K |
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* pmb = double (Given) |
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* Ambient pressure, millibars |
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* rh = double (Given) |
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* Ambient relative humidity, 0-1 |
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* wl1 = double (Given) |
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* Reference wavelength, micrometre (0.4 recommended) |
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* a1 = double (Given) |
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* Refraction coefficient A for wavelength wl1 (radians) |
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* b1 = double (Given) |
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* Refraction coefficient B for wavelength wl1 (radians) |
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* wl2 = double (Given) |
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* Wavelength for which adjusted A,B required |
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* a2 = double * (Returned) |
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* Refraction coefficient A for wavelength WL2 (radians) |
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* b2 = double * (Returned) |
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* Refraction coefficient B for wavelength WL2 (radians) |
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* Description: |
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* Apply atmospheric-dispersion adjustments to refraction coefficients. |
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* Authors: |
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* TIMJ: Tim Jenness |
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* PTW: Patrick Wallace |
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* {enter_new_authors_here} |
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* Notes: |
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* - To use this routine, first call palRefco specifying WL1 as the |
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* wavelength. This yields refraction coefficients A1,B1, correct |
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* for that wavelength. Subsequently, calls to palAtmdsp specifying |
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* different wavelengths will produce new, slightly adjusted |
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* refraction coefficients which apply to the specified wavelength. |
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* |
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* - Most of the atmospheric dispersion happens between 0.7 micrometre |
56
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* and the UV atmospheric cutoff, and the effect increases strongly |
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* towards the UV end. For this reason a blue reference wavelength |
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* is recommended, for example 0.4 micrometres. |
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* |
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* - The accuracy, for this set of conditions: |
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* |
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* height above sea level 2000 m |
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* latitude 29 deg |
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* pressure 793 mb |
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* temperature 17 degC |
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* humidity 50% |
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* lapse rate 0.0065 degC/m |
68
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* reference wavelength 0.4 micrometre |
69
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* star elevation 15 deg |
70
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* |
71
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* is about 2.5 mas RMS between 0.3 and 1.0 micrometres, and stays |
72
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* within 4 mas for the whole range longward of 0.3 micrometres |
73
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* (compared with a total dispersion from 0.3 to 20.0 micrometres |
74
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* of about 11 arcsec). These errors are typical for ordinary |
75
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* conditions and the given elevation; in extreme conditions values |
76
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* a few times this size may occur, while at higher elevations the |
77
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* errors become much smaller. |
78
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* |
79
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* - If either wavelength exceeds 100 micrometres, the radio case |
80
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* is assumed and the returned refraction coefficients are the |
81
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* same as the given ones. Note that radio refraction coefficients |
82
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* cannot be turned into optical values using this routine, nor |
83
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* vice versa. |
84
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* |
85
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* - The algorithm consists of calculation of the refractivity of the |
86
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* air at the observer for the two wavelengths, using the methods |
87
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* of the palRefro routine, and then scaling of the two refraction |
88
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* coefficients according to classical refraction theory. This |
89
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* amounts to scaling the A coefficient in proportion to (n-1) and |
90
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* the B coefficient almost in the same ratio (see R.M.Green, |
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* "Spherical Astronomy", Cambridge University Press, 1985). |
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93
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* History: |
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* 2014-07-15 (TIMJ): |
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* Initial version. A direct copy of the Fortran SLA implementation. |
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* Adapted with permission from the Fortran SLALIB library. |
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* {enter_further_changes_here} |
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99
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* Copyright: |
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* Copyright (C) 2014 Tim Jenness |
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* Copyright (C) 2005 Patrick Wallace |
102
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* All Rights Reserved. |
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104
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* Licence: |
105
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* This program is free software; you can redistribute it and/or |
106
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* modify it under the terms of the GNU General Public License as |
107
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* published by the Free Software Foundation; either version 3 of |
108
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* the License, or (at your option) any later version. |
109
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* |
110
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* This program is distributed in the hope that it will be |
111
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* useful, but WITHOUT ANY WARRANTY; without even the implied |
112
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* warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR |
113
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* PURPOSE. See the GNU General Public License for more details. |
114
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* |
115
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* You should have received a copy of the GNU General Public License |
116
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* along with this program; if not, write to the Free Software |
117
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* Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, |
118
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* MA 02110-1301, USA. |
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120
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* Bugs: |
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* {note_any_bugs_here} |
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*- |
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*/ |
124
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125
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#include "pal.h" |
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#include "palmac.h" |
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#include |
128
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129
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1
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void palAtmdsp ( double tdk, double pmb, double rh, double wl1, |
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double a1, double b1, double wl2, double *a2, double *b2 ) { |
131
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132
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double f,tdkok,pmbok,rhok; |
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double psat,pwo,w1,wlok,wlsq,w2,dn1,dn2; |
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135
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/* Check for radio wavelengths */ |
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1
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50
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if (wl1 > 100.0 || wl2 > 100.0) { |
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50
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137
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138
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/* Radio: no dispersion */ |
139
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0
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*a2 = a1; |
140
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0
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*b2 = b1; |
141
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142
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} else { |
143
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144
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/* Optical: keep arguments within safe bounds */ |
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1
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50
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tdkok = DMIN(DMAX(tdk,100.0),500.0); |
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50
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50
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146
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1
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50
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pmbok = DMIN(DMAX(pmb,0.0),10000.0); |
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50
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50
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147
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1
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50
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rhok = DMIN(DMAX(rh,0.0),1.0); |
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50
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50
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148
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149
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/* Atmosphere parameters at the observer */ |
150
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1
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psat = pow(10.0, -8.7115+0.03477*tdkok); |
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1
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pwo = rhok*psat; |
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1
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w1 = 11.2684e-6*pwo; |
153
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154
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/* Refractivity at the observer for first wavelength */ |
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1
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50
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wlok = DMAX(wl1,0.1); |
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1
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wlsq = wlok*wlok; |
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1
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w2 = 77.5317e-6+(0.43909e-6+0.00367e-6/wlsq)/wlsq; |
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1
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dn1 = (w2*pmbok-w1)/tdkok; |
159
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160
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/* Refractivity at the observer for second wavelength */ |
161
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1
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50
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wlok = DMAX(wl2,0.1); |
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1
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wlsq = wlok*wlok; |
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1
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w2 = 77.5317e-6+(0.43909e-6+0.00367e-6/wlsq)/wlsq; |
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1
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dn2 = (w2*pmbok-w1)/tdkok; |
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166
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/* Scale the refraction coefficients (see Green 4.31, p93) */ |
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1
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50
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if (dn1 != 0.0) { |
168
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1
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f = dn2/dn1; |
169
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1
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*a2 = a1*f; |
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1
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*b2 = b1*f; |
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1
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50
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if (dn1 != a1) { |
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1
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*b2 *= (1.0+dn1*(dn1-dn2)/(2.0*(dn1-a1))); |
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} |
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} else { |
175
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0
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*a2 = a1; |
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0
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*b2 = b1; |
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} |
178
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} |
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180
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1
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} |