| 1 | #include "erfa.h"
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| 2 |
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| 3 | void eraPrec76(double date01, double date02, double date11, double date12,
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| 4 | double *zeta, double *z, double *theta)
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| 5 | /*
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| 6 | ** - - - - - - - - - -
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| 7 | ** e r a P r e c 7 6
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| 8 | ** - - - - - - - - - -
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| 9 | **
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| 10 | ** IAU 1976 precession model.
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| 11 | **
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| 12 | ** This function forms the three Euler angles which implement general
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| 13 | ** precession between two dates, using the IAU 1976 model (as for the
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| 14 | ** FK5 catalog).
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| 15 | **
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| 16 | ** Given:
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| 17 | ** date01,date02 double TDB starting date (Note 1)
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| 18 | ** date11,date12 double TDB ending date (Note 1)
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| 19 | **
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| 20 | ** Returned:
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| 21 | ** zeta double 1st rotation: radians cw around z
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| 22 | ** z double 3rd rotation: radians cw around z
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| 23 | ** theta double 2nd rotation: radians ccw around y
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| 24 | **
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| 25 | ** Notes:
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| 26 | **
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| 27 | ** 1) The dates date01+date02 and date11+date12 are Julian Dates,
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| 28 | ** apportioned in any convenient way between the arguments daten1
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| 29 | ** and daten2. For example, JD(TDB)=2450123.7 could be expressed in
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| 30 | ** any of these ways, among others:
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| 31 | **
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| 32 | ** daten1 daten2
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| 33 | **
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| 34 | ** 2450123.7 0.0 (JD method)
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| 35 | ** 2451545.0 -1421.3 (J2000 method)
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| 36 | ** 2400000.5 50123.2 (MJD method)
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| 37 | ** 2450123.5 0.2 (date & time method)
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| 38 | **
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| 39 | ** The JD method is the most natural and convenient to use in cases
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| 40 | ** where the loss of several decimal digits of resolution is
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| 41 | ** acceptable. The J2000 method is best matched to the way the
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| 42 | ** argument is handled internally and will deliver the optimum
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| 43 | ** optimum resolution. The MJD method and the date & time methods
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| 44 | ** are both good compromises between resolution and convenience.
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| 45 | ** The two dates may be expressed using different methods, but at
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| 46 | ** the risk of losing some resolution.
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| 47 | **
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| 48 | ** 2) The accumulated precession angles zeta, z, theta are expressed
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| 49 | ** through canonical polynomials which are valid only for a limited
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| 50 | ** time span. In addition, the IAU 1976 precession rate is known to
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| 51 | ** be imperfect. The absolute accuracy of the present formulation
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| 52 | ** is better than 0.1 arcsec from 1960AD to 2040AD, better than
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| 53 | ** 1 arcsec from 1640AD to 2360AD, and remains below 3 arcsec for
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| 54 | ** the whole of the period 500BC to 3000AD. The errors exceed
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| 55 | ** 10 arcsec outside the range 1200BC to 3900AD, exceed 100 arcsec
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| 56 | ** outside 4200BC to 5600AD and exceed 1000 arcsec outside 6800BC to
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| 57 | ** 8200AD.
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| 58 | **
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| 59 | ** 3) The three angles are returned in the conventional order, which
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| 60 | ** is not the same as the order of the corresponding Euler
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| 61 | ** rotations. The precession matrix is
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| 62 | ** R_3(-z) x R_2(+theta) x R_3(-zeta).
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| 63 | **
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| 64 | ** Reference:
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| 65 | **
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| 66 | ** Lieske, J.H., 1979, Astron.Astrophys. 73, 282, equations
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| 67 | ** (6) & (7), p283.
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| 68 | **
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| 69 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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| 70 | ** Derived, with permission, from the SOFA library. See notes at end of file.
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| 71 | */
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| 72 | {
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| 73 | double t0, t, tas2r, w;
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| 74 |
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| 75 |
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| 76 | /* Interval between fundamental epoch J2000.0 and start date (JC). */
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| 77 | t0 = ((date01 - ERFA_DJ00) + date02) / ERFA_DJC;
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| 78 |
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| 79 | /* Interval over which precession required (JC). */
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| 80 | t = ((date11 - date01) + (date12 - date02)) / ERFA_DJC;
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| 81 |
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| 82 | /* Euler angles. */
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| 83 | tas2r = t * ERFA_DAS2R;
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| 84 | w = 2306.2181 + (1.39656 - 0.000139 * t0) * t0;
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| 85 |
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| 86 | *zeta = (w + ((0.30188 - 0.000344 * t0) + 0.017998 * t) * t) * tas2r;
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| 87 |
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| 88 | *z = (w + ((1.09468 + 0.000066 * t0) + 0.018203 * t) * t) * tas2r;
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| 89 |
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| 90 | *theta = ((2004.3109 + (-0.85330 - 0.000217 * t0) * t0)
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| 91 | + ((-0.42665 - 0.000217 * t0) - 0.041833 * t) * t) * tas2r;
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| 92 |
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| 93 | return;
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| 94 |
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| 95 | }
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| 96 | /*----------------------------------------------------------------------
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| 97 | **
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| 98 | **
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| 99 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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| 100 | ** All rights reserved.
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| 101 | **
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| 102 | ** This library is derived, with permission, from the International
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| 103 | ** Astronomical Union's "Standards of Fundamental Astronomy" library,
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| 104 | ** available from http://www.iausofa.org.
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| 105 | **
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| 106 | ** The ERFA version is intended to retain identical functionality to
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| 107 | ** the SOFA library, but made distinct through different function and
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| 108 | ** file names, as set out in the SOFA license conditions. The SOFA
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| 109 | ** original has a role as a reference standard for the IAU and IERS,
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| 110 | ** and consequently redistribution is permitted only in its unaltered
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| 111 | ** state. The ERFA version is not subject to this restriction and
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| 112 | ** therefore can be included in distributions which do not support the
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| 113 | ** concept of "read only" software.
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| 114 | **
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| 115 | ** Although the intent is to replicate the SOFA API (other than
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| 116 | ** replacement of prefix names) and results (with the exception of
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| 117 | ** bugs; any that are discovered will be fixed), SOFA is not
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| 118 | ** responsible for any errors found in this version of the library.
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| 119 | **
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| 120 | ** If you wish to acknowledge the SOFA heritage, please acknowledge
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| 121 | ** that you are using a library derived from SOFA, rather than SOFA
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| 122 | ** itself.
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| 123 | **
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| 124 | **
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| 125 | ** TERMS AND CONDITIONS
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| 126 | **
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| 127 | ** Redistribution and use in source and binary forms, with or without
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| 128 | ** modification, are permitted provided that the following conditions
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| 129 | ** are met:
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| 130 | **
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| 131 | ** 1 Redistributions of source code must retain the above copyright
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| 132 | ** notice, this list of conditions and the following disclaimer.
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| 133 | **
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| 134 | ** 2 Redistributions in binary form must reproduce the above copyright
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| 135 | ** notice, this list of conditions and the following disclaimer in
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| 136 | ** the documentation and/or other materials provided with the
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| 137 | ** distribution.
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| 138 | **
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| 139 | ** 3 Neither the name of the Standards Of Fundamental Astronomy Board,
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| 140 | ** the International Astronomical Union nor the names of its
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| 141 | ** contributors may be used to endorse or promote products derived
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| 142 | ** from this software without specific prior written permission.
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| 143 | **
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| 144 | ** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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| 145 | ** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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| 146 | ** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
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| 147 | ** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
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| 148 | ** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
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| 149 | ** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
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| 150 | ** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
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| 151 | ** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
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| 152 | ** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
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| 153 | ** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
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| 154 | ** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
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| 155 | ** POSSIBILITY OF SUCH DAMAGE.
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| 156 | **
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| 157 | */
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