1 #include "erfa.h"
2 
eraAtoc13(const char * type,double ob1,double ob2,double utc1,double utc2,double dut1,double elong,double phi,double hm,double xp,double yp,double phpa,double tc,double rh,double wl,double * rc,double * dc)3 int eraAtoc13(const char *type, double ob1, double ob2,
4               double utc1, double utc2, double dut1,
5               double elong, double phi, double hm, double xp, double yp,
6               double phpa, double tc, double rh, double wl,
7               double *rc, double *dc)
8 /*
9 **  - - - - - - - - - -
10 **   e r a A t o c 1 3
11 **  - - - - - - - - - -
12 **
13 **  Observed place at a groundbased site to to ICRS astrometric RA,Dec.
14 **  The caller supplies UTC, site coordinates, ambient air conditions
15 **  and observing wavelength.
16 **
17 **  Given:
18 **     type   char[]   type of coordinates - "R", "H" or "A" (Notes 1,2)
19 **     ob1    double   observed Az, HA or RA (radians; Az is N=0,E=90)
20 **     ob2    double   observed ZD or Dec (radians)
21 **     utc1   double   UTC as a 2-part...
22 **     utc2   double   ...quasi Julian Date (Notes 3,4)
23 **     dut1   double   UT1-UTC (seconds, Note 5)
24 **     elong  double   longitude (radians, east +ve, Note 6)
25 **     phi    double   geodetic latitude (radians, Note 6)
26 **     hm     double   height above ellipsoid (m, geodetic Notes 6,8)
27 **     xp,yp  double   polar motion coordinates (radians, Note 7)
28 **     phpa   double   pressure at the observer (hPa = mB, Note 8)
29 **     tc     double   ambient temperature at the observer (deg C)
30 **     rh     double   relative humidity at the observer (range 0-1)
31 **     wl     double   wavelength (micrometers, Note 9)
32 **
33 **  Returned:
34 **     rc,dc  double   ICRS astrometric RA,Dec (radians)
35 **
36 **  Returned (function value):
37 **            int      status: +1 = dubious year (Note 4)
38 **                              0 = OK
39 **                             -1 = unacceptable date
40 **
41 **  Notes:
42 **
43 **  1)  "Observed" Az,ZD means the position that would be seen by a
44 **      perfect geodetically aligned theodolite.  (Zenith distance is
45 **      used rather than altitude in order to reflect the fact that no
46 **      allowance is made for depression of the horizon.)  This is
47 **      related to the observed HA,Dec via the standard rotation, using
48 **      the geodetic latitude (corrected for polar motion), while the
49 **      observed HA and RA are related simply through the Earth rotation
50 **      angle and the site longitude.  "Observed" RA,Dec or HA,Dec thus
51 **      means the position that would be seen by a perfect equatorial
52 **      with its polar axis aligned to the Earth's axis of rotation.
53 **
54 **  2)  Only the first character of the type argument is significant.
55 **      "R" or "r" indicates that ob1 and ob2 are the observed right
56 **      ascension and declination;  "H" or "h" indicates that they are
57 **      hour angle (west +ve) and declination;  anything else ("A" or
58 **      "a" is recommended) indicates that ob1 and ob2 are azimuth
59 **      (north zero, east 90 deg) and zenith distance.
60 **
61 **  3)  utc1+utc2 is quasi Julian Date (see Note 2), apportioned in any
62 **      convenient way between the two arguments, for example where utc1
63 **      is the Julian Day Number and utc2 is the fraction of a day.
64 **
65 **      However, JD cannot unambiguously represent UTC during a leap
66 **      second unless special measures are taken.  The convention in the
67 **      present function is that the JD day represents UTC days whether
68 **      the length is 86399, 86400 or 86401 SI seconds.
69 **
70 **      Applications should use the function eraDtf2d to convert from
71 **      calendar date and time of day into 2-part quasi Julian Date, as
72 **      it implements the leap-second-ambiguity convention just
73 **      described.
74 **
75 **  4)  The warning status "dubious year" flags UTCs that predate the
76 **      introduction of the time scale or that are too far in the
77 **      future to be trusted.  See eraDat for further details.
78 **
79 **  5)  UT1-UTC is tabulated in IERS bulletins.  It increases by exactly
80 **      one second at the end of each positive UTC leap second,
81 **      introduced in order to keep UT1-UTC within +/- 0.9s.  n.b. This
82 **      practice is under review, and in the future UT1-UTC may grow
83 **      essentially without limit.
84 **
85 **  6)  The geographical coordinates are with respect to the ERFA_WGS84
86 **      reference ellipsoid.  TAKE CARE WITH THE LONGITUDE SIGN:  the
87 **      longitude required by the present function is east-positive
88 **      (i.e. right-handed), in accordance with geographical convention.
89 **
90 **  7)  The polar motion xp,yp can be obtained from IERS bulletins.  The
91 **      values are the coordinates (in radians) of the Celestial
92 **      Intermediate Pole with respect to the International Terrestrial
93 **      Reference System (see IERS Conventions 2003), measured along the
94 **      meridians 0 and 90 deg west respectively.  For many
95 **      applications, xp and yp can be set to zero.
96 **
97 **  8)  If hm, the height above the ellipsoid of the observing station
98 **      in meters, is not known but phpa, the pressure in hPa (=mB), is
99 **      available, an adequate estimate of hm can be obtained from the
100 **      expression
101 **
102 **            hm = -29.3 * tsl * log ( phpa / 1013.25 );
103 **
104 **      where tsl is the approximate sea-level air temperature in K
105 **      (See Astrophysical Quantities, C.W.Allen, 3rd edition, section
106 **      52).  Similarly, if the pressure phpa is not known, it can be
107 **      estimated from the height of the observing station, hm, as
108 **      follows:
109 **
110 **            phpa = 1013.25 * exp ( -hm / ( 29.3 * tsl ) );
111 **
112 **      Note, however, that the refraction is nearly proportional to
113 **      the pressure and that an accurate phpa value is important for
114 **      precise work.
115 **
116 **  9)  The argument wl specifies the observing wavelength in
117 **      micrometers.  The transition from optical to radio is assumed to
118 **      occur at 100 micrometers (about 3000 GHz).
119 **
120 **  10) The accuracy of the result is limited by the corrections for
121 **      refraction, which use a simple A*tan(z) + B*tan^3(z) model.
122 **      Providing the meteorological parameters are known accurately and
123 **      there are no gross local effects, the predicted astrometric
124 **      coordinates should be within 0.05 arcsec (optical) or 1 arcsec
125 **      (radio) for a zenith distance of less than 70 degrees, better
126 **      than 30 arcsec (optical or radio) at 85 degrees and better
127 **      than 20 arcmin (optical) or 30 arcmin (radio) at the horizon.
128 **
129 **      Without refraction, the complementary functions eraAtco13 and
130 **      eraAtoc13 are self-consistent to better than 1 microarcsecond
131 **      all over the celestial sphere.  With refraction included,
132 **      consistency falls off at high zenith distances, but is still
133 **      better than 0.05 arcsec at 85 degrees.
134 **
135 **  11) It is advisable to take great care with units, as even unlikely
136 **      values of the input parameters are accepted and processed in
137 **      accordance with the models used.
138 **
139 **  Called:
140 **     eraApco13    astrometry parameters, ICRS-observed
141 **     eraAtoiq     quick observed to CIRS
142 **     eraAticq     quick CIRS to ICRS
143 **
144 **  Copyright (C) 2013-2020, NumFOCUS Foundation.
145 **  Derived, with permission, from the SOFA library.  See notes at end of file.
146 */
147 {
148    int j;
149    eraASTROM astrom;
150    double eo, ri, di;
151 
152 
153 /* Star-independent astrometry parameters. */
154    j = eraApco13(utc1, utc2, dut1, elong, phi, hm, xp, yp,
155                  phpa, tc, rh, wl, &astrom, &eo);
156 
157 /* Abort if bad UTC. */
158    if ( j < 0 ) return j;
159 
160 /* Transform observed to CIRS. */
161    eraAtoiq(type, ob1, ob2, &astrom, &ri, &di);
162 
163 /* Transform CIRS to ICRS. */
164    eraAticq(ri, di, &astrom, rc, dc);
165 
166 /* Return OK/warning status. */
167    return j;
168 
169 /* Finished. */
170 
171 }
172 /*----------------------------------------------------------------------
173 **
174 **
175 **  Copyright (C) 2013-2020, NumFOCUS Foundation.
176 **  All rights reserved.
177 **
178 **  This library is derived, with permission, from the International
179 **  Astronomical Union's "Standards of Fundamental Astronomy" library,
180 **  available from http://www.iausofa.org.
181 **
182 **  The ERFA version is intended to retain identical functionality to
183 **  the SOFA library, but made distinct through different function and
184 **  file names, as set out in the SOFA license conditions.  The SOFA
185 **  original has a role as a reference standard for the IAU and IERS,
186 **  and consequently redistribution is permitted only in its unaltered
187 **  state.  The ERFA version is not subject to this restriction and
188 **  therefore can be included in distributions which do not support the
189 **  concept of "read only" software.
190 **
191 **  Although the intent is to replicate the SOFA API (other than
192 **  replacement of prefix names) and results (with the exception of
193 **  bugs;  any that are discovered will be fixed), SOFA is not
194 **  responsible for any errors found in this version of the library.
195 **
196 **  If you wish to acknowledge the SOFA heritage, please acknowledge
197 **  that you are using a library derived from SOFA, rather than SOFA
198 **  itself.
199 **
200 **
201 **  TERMS AND CONDITIONS
202 **
203 **  Redistribution and use in source and binary forms, with or without
204 **  modification, are permitted provided that the following conditions
205 **  are met:
206 **
207 **  1 Redistributions of source code must retain the above copyright
208 **    notice, this list of conditions and the following disclaimer.
209 **
210 **  2 Redistributions in binary form must reproduce the above copyright
211 **    notice, this list of conditions and the following disclaimer in
212 **    the documentation and/or other materials provided with the
213 **    distribution.
214 **
215 **  3 Neither the name of the Standards Of Fundamental Astronomy Board,
216 **    the International Astronomical Union nor the names of its
217 **    contributors may be used to endorse or promote products derived
218 **    from this software without specific prior written permission.
219 **
220 **  THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
221 **  "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
222 **  LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
223 **  FOR A PARTICULAR PURPOSE ARE DISCLAIMED.  IN NO EVENT SHALL THE
224 **  COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
225 **  INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
226 **  BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
227 **  LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
228 **  CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
229 **  LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
230 **  ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
231 **  POSSIBILITY OF SUCH DAMAGE.
232 **
233 */
234