1 #include "erfa.h"
2 
eraC2tpe(double tta,double ttb,double uta,double utb,double dpsi,double deps,double xp,double yp,double rc2t[3][3])3 void eraC2tpe(double tta, double ttb, double uta, double utb,
4               double dpsi, double deps, double xp, double yp,
5               double rc2t[3][3])
6 /*
7 **  - - - - - - - - -
8 **   e r a C 2 t p e
9 **  - - - - - - - - -
10 **
11 **  Form the celestial to terrestrial matrix given the date, the UT1,
12 **  the nutation and the polar motion.  IAU 2000.
13 **
14 **  Given:
15 **     tta,ttb    double        TT as a 2-part Julian Date (Note 1)
16 **     uta,utb    double        UT1 as a 2-part Julian Date (Note 1)
17 **     dpsi,deps  double        nutation (Note 2)
18 **     xp,yp      double        coordinates of the pole (radians, Note 3)
19 **
20 **  Returned:
21 **     rc2t       double[3][3]  celestial-to-terrestrial matrix (Note 4)
22 **
23 **  Notes:
24 **
25 **  1) The TT and UT1 dates tta+ttb and uta+utb are Julian Dates,
26 **     apportioned in any convenient way between the arguments uta and
27 **     utb.  For example, JD(UT1)=2450123.7 could be expressed in any of
28 **     these ways, among others:
29 **
30 **             uta            utb
31 **
32 **         2450123.7           0.0       (JD method)
33 **         2451545.0       -1421.3       (J2000 method)
34 **         2400000.5       50123.2       (MJD method)
35 **         2450123.5           0.2       (date & time method)
36 **
37 **     The JD method is the most natural and convenient to use in
38 **     cases where the loss of several decimal digits of resolution is
39 **     acceptable.  The J2000 and MJD methods are good compromises
40 **     between resolution and convenience.  In the case of uta,utb, the
41 **     date & time method is best matched to the Earth rotation angle
42 **     algorithm used:  maximum precision is delivered when the uta
43 **     argument is for 0hrs UT1 on the day in question and the utb
44 **     argument lies in the range 0 to 1, or vice versa.
45 **
46 **  2) The caller is responsible for providing the nutation components;
47 **     they are in longitude and obliquity, in radians and are with
48 **     respect to the equinox and ecliptic of date.  For high-accuracy
49 **     applications, free core nutation should be included as well as
50 **     any other relevant corrections to the position of the CIP.
51 **
52 **  3) The arguments xp and yp are the coordinates (in radians) of the
53 **     Celestial Intermediate Pole with respect to the International
54 **     Terrestrial Reference System (see IERS Conventions 2003),
55 **     measured along the meridians to 0 and 90 deg west respectively.
56 **
57 **  4) The matrix rc2t transforms from celestial to terrestrial
58 **     coordinates:
59 **
60 **        [TRS] = RPOM * R_3(GST) * RBPN * [CRS]
61 **
62 **              = rc2t * [CRS]
63 **
64 **     where [CRS] is a vector in the Geocentric Celestial Reference
65 **     System and [TRS] is a vector in the International Terrestrial
66 **     Reference System (see IERS Conventions 2003), RBPN is the
67 **     bias-precession-nutation matrix, GST is the Greenwich (apparent)
68 **     Sidereal Time and RPOM is the polar motion matrix.
69 **
70 **  5) Although its name does not include "00", This function is in fact
71 **     specific to the IAU 2000 models.
72 **
73 **  Called:
74 **     eraPn00      bias/precession/nutation results, IAU 2000
75 **     eraGmst00    Greenwich mean sidereal time, IAU 2000
76 **     eraSp00      the TIO locator s', IERS 2000
77 **     eraEe00      equation of the equinoxes, IAU 2000
78 **     eraPom00     polar motion matrix
79 **     eraC2teqx    form equinox-based celestial-to-terrestrial matrix
80 **
81 **  Reference:
82 **
83 **     McCarthy, D. D., Petit, G. (eds.), IERS Conventions (2003),
84 **     IERS Technical Note No. 32, BKG (2004)
85 **
86 **  Copyright (C) 2013-2020, NumFOCUS Foundation.
87 **  Derived, with permission, from the SOFA library.  See notes at end of file.
88 */
89 {
90    double epsa, rb[3][3], rp[3][3], rbp[3][3], rn[3][3],
91           rbpn[3][3], gmst, ee, sp, rpom[3][3];
92 
93 
94 /* Form the celestial-to-true matrix for this TT. */
95    eraPn00(tta, ttb, dpsi, deps, &epsa, rb, rp, rbp, rn, rbpn);
96 
97 /* Predict the Greenwich Mean Sidereal Time for this UT1 and TT. */
98    gmst = eraGmst00(uta, utb, tta, ttb);
99 
100 /* Predict the equation of the equinoxes given TT and nutation. */
101    ee = eraEe00(tta, ttb, epsa, dpsi);
102 
103 /* Estimate s'. */
104    sp = eraSp00(tta, ttb);
105 
106 /* Form the polar motion matrix. */
107    eraPom00(xp, yp, sp, rpom);
108 
109 /* Combine to form the celestial-to-terrestrial matrix. */
110    eraC2teqx(rbpn, gmst + ee, rpom, rc2t);
111 
112    return;
113 
114 }
115 /*----------------------------------------------------------------------
116 **
117 **
118 **  Copyright (C) 2013-2020, NumFOCUS Foundation.
119 **  All rights reserved.
120 **
121 **  This library is derived, with permission, from the International
122 **  Astronomical Union's "Standards of Fundamental Astronomy" library,
123 **  available from http://www.iausofa.org.
124 **
125 **  The ERFA version is intended to retain identical functionality to
126 **  the SOFA library, but made distinct through different function and
127 **  file names, as set out in the SOFA license conditions.  The SOFA
128 **  original has a role as a reference standard for the IAU and IERS,
129 **  and consequently redistribution is permitted only in its unaltered
130 **  state.  The ERFA version is not subject to this restriction and
131 **  therefore can be included in distributions which do not support the
132 **  concept of "read only" software.
133 **
134 **  Although the intent is to replicate the SOFA API (other than
135 **  replacement of prefix names) and results (with the exception of
136 **  bugs;  any that are discovered will be fixed), SOFA is not
137 **  responsible for any errors found in this version of the library.
138 **
139 **  If you wish to acknowledge the SOFA heritage, please acknowledge
140 **  that you are using a library derived from SOFA, rather than SOFA
141 **  itself.
142 **
143 **
144 **  TERMS AND CONDITIONS
145 **
146 **  Redistribution and use in source and binary forms, with or without
147 **  modification, are permitted provided that the following conditions
148 **  are met:
149 **
150 **  1 Redistributions of source code must retain the above copyright
151 **    notice, this list of conditions and the following disclaimer.
152 **
153 **  2 Redistributions in binary form must reproduce the above copyright
154 **    notice, this list of conditions and the following disclaimer in
155 **    the documentation and/or other materials provided with the
156 **    distribution.
157 **
158 **  3 Neither the name of the Standards Of Fundamental Astronomy Board,
159 **    the International Astronomical Union nor the names of its
160 **    contributors may be used to endorse or promote products derived
161 **    from this software without specific prior written permission.
162 **
163 **  THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
164 **  "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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166 **  FOR A PARTICULAR PURPOSE ARE DISCLAIMED.  IN NO EVENT SHALL THE
167 **  COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
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176 */
177