1 #include "erfa.h"
2 
eraApio13(double utc1,double utc2,double dut1,double elong,double phi,double hm,double xp,double yp,double phpa,double tc,double rh,double wl,eraASTROM * astrom)3 int eraApio13(double utc1, double utc2, double dut1,
4               double elong, double phi, double hm, double xp, double yp,
5               double phpa, double tc, double rh, double wl,
6               eraASTROM *astrom)
7 /*
8 **  - - - - - - - - - -
9 **   e r a A p i o 1 3
10 **  - - - - - - - - - -
11 **
12 **  For a terrestrial observer, prepare star-independent astrometry
13 **  parameters for transformations between CIRS and observed
14 **  coordinates.  The caller supplies UTC, site coordinates, ambient air
15 **  conditions and observing wavelength.
16 **
17 **  Given:
18 **     utc1   double      UTC as a 2-part...
19 **     utc2   double      ...quasi Julian Date (Notes 1,2)
20 **     dut1   double      UT1-UTC (seconds)
21 **     elong  double      longitude (radians, east +ve, Note 3)
22 **     phi    double      geodetic latitude (radians, Note 3)
23 **     hm     double      height above ellipsoid (m, geodetic Notes 4,6)
24 **     xp,yp  double      polar motion coordinates (radians, Note 5)
25 **     phpa   double      pressure at the observer (hPa = mB, Note 6)
26 **     tc     double      ambient temperature at the observer (deg C)
27 **     rh     double      relative humidity at the observer (range 0-1)
28 **     wl     double      wavelength (micrometers, Note 7)
29 **
30 **  Returned:
31 **     astrom eraASTROM*  star-independent astrometry parameters:
32 **      pmt    double       unchanged
33 **      eb     double[3]    unchanged
34 **      eh     double[3]    unchanged
35 **      em     double       unchanged
36 **      v      double[3]    unchanged
37 **      bm1    double       unchanged
38 **      bpn    double[3][3] unchanged
39 **      along  double       longitude + s' (radians)
40 **      xpl    double       polar motion xp wrt local meridian (radians)
41 **      ypl    double       polar motion yp wrt local meridian (radians)
42 **      sphi   double       sine of geodetic latitude
43 **      cphi   double       cosine of geodetic latitude
44 **      diurab double       magnitude of diurnal aberration vector
45 **      eral   double       "local" Earth rotation angle (radians)
46 **      refa   double       refraction constant A (radians)
47 **      refb   double       refraction constant B (radians)
48 **
49 **  Returned (function value):
50 **            int         status: +1 = dubious year (Note 2)
51 **                                 0 = OK
52 **                                -1 = unacceptable date
53 **
54 **  Notes:
55 **
56 **  1)  utc1+utc2 is quasi Julian Date (see Note 2), apportioned in any
57 **      convenient way between the two arguments, for example where utc1
58 **      is the Julian Day Number and utc2 is the fraction of a day.
59 **
60 **      However, JD cannot unambiguously represent UTC during a leap
61 **      second unless special measures are taken.  The convention in the
62 **      present function is that the JD day represents UTC days whether
63 **      the length is 86399, 86400 or 86401 SI seconds.
64 **
65 **      Applications should use the function eraDtf2d to convert from
66 **      calendar date and time of day into 2-part quasi Julian Date, as
67 **      it implements the leap-second-ambiguity convention just
68 **      described.
69 **
70 **  2)  The warning status "dubious year" flags UTCs that predate the
71 **      introduction of the time scale or that are too far in the future
72 **      to be trusted.  See eraDat for further details.
73 **
74 **  3)  UT1-UTC is tabulated in IERS bulletins.  It increases by exactly
75 **      one second at the end of each positive UTC leap second,
76 **      introduced in order to keep UT1-UTC within +/- 0.9s.  n.b. This
77 **      practice is under review, and in the future UT1-UTC may grow
78 **      essentially without limit.
79 **
80 **  4)  The geographical coordinates are with respect to the ERFA_WGS84
81 **      reference ellipsoid.  TAKE CARE WITH THE LONGITUDE SIGN:  the
82 **      longitude required by the present function is east-positive
83 **      (i.e. right-handed), in accordance with geographical convention.
84 **
85 **  5)  The polar motion xp,yp can be obtained from IERS bulletins.  The
86 **      values are the coordinates (in radians) of the Celestial
87 **      Intermediate Pole with respect to the International Terrestrial
88 **      Reference System (see IERS Conventions 2003), measured along the
89 **      meridians 0 and 90 deg west respectively.  For many applications,
90 **      xp and yp can be set to zero.
91 **
92 **      Internally, the polar motion is stored in a form rotated onto
93 **      the local meridian.
94 **
95 **  6)  If hm, the height above the ellipsoid of the observing station
96 **      in meters, is not known but phpa, the pressure in hPa (=mB), is
97 **      available, an adequate estimate of hm can be obtained from the
98 **      expression
99 **
100 **            hm = -29.3 * tsl * log ( phpa / 1013.25 );
101 **
102 **      where tsl is the approximate sea-level air temperature in K
103 **      (See Astrophysical Quantities, C.W.Allen, 3rd edition, section
104 **      52).  Similarly, if the pressure phpa is not known, it can be
105 **      estimated from the height of the observing station, hm, as
106 **      follows:
107 **
108 **            phpa = 1013.25 * exp ( -hm / ( 29.3 * tsl ) );
109 **
110 **      Note, however, that the refraction is nearly proportional to the
111 **      pressure and that an accurate phpa value is important for
112 **      precise work.
113 **
114 **  7)  The argument wl specifies the observing wavelength in
115 **      micrometers.  The transition from optical to radio is assumed to
116 **      occur at 100 micrometers (about 3000 GHz).
117 **
118 **  8)  It is advisable to take great care with units, as even unlikely
119 **      values of the input parameters are accepted and processed in
120 **      accordance with the models used.
121 **
122 **  9)  In cases where the caller wishes to supply his own Earth
123 **      rotation information and refraction constants, the function
124 **      eraApc can be used instead of the present function.
125 **
126 **  10) This is one of several functions that inserts into the astrom
127 **      structure star-independent parameters needed for the chain of
128 **      astrometric transformations ICRS <-> GCRS <-> CIRS <-> observed.
129 **
130 **      The various functions support different classes of observer and
131 **      portions of the transformation chain:
132 **
133 **          functions         observer        transformation
134 **
135 **       eraApcg eraApcg13    geocentric      ICRS <-> GCRS
136 **       eraApci eraApci13    terrestrial     ICRS <-> CIRS
137 **       eraApco eraApco13    terrestrial     ICRS <-> observed
138 **       eraApcs eraApcs13    space           ICRS <-> GCRS
139 **       eraAper eraAper13    terrestrial     update Earth rotation
140 **       eraApio eraApio13    terrestrial     CIRS <-> observed
141 **
142 **      Those with names ending in "13" use contemporary ERFA models to
143 **      compute the various ephemerides.  The others accept ephemerides
144 **      supplied by the caller.
145 **
146 **      The transformation from ICRS to GCRS covers space motion,
147 **      parallax, light deflection, and aberration.  From GCRS to CIRS
148 **      comprises frame bias and precession-nutation.  From CIRS to
149 **      observed takes account of Earth rotation, polar motion, diurnal
150 **      aberration and parallax (unless subsumed into the ICRS <-> GCRS
151 **      transformation), and atmospheric refraction.
152 **
153 **  11) The context structure astrom produced by this function is used
154 **      by eraAtioq and eraAtoiq.
155 **
156 **  Called:
157 **     eraUtctai    UTC to TAI
158 **     eraTaitt     TAI to TT
159 **     eraUtcut1    UTC to UT1
160 **     eraSp00      the TIO locator s', IERS 2000
161 **     eraEra00     Earth rotation angle, IAU 2000
162 **     eraRefco     refraction constants for given ambient conditions
163 **     eraApio      astrometry parameters, CIRS-observed
164 **
165 **  Copyright (C) 2013-2014, NumFOCUS Foundation.
166 **  Derived, with permission, from the SOFA library.  See notes at end of file.
167 */
168 {
169    int j;
170    double tai1, tai2, tt1, tt2, ut11, ut12, sp, theta, refa, refb;
171 
172 
173 /* UTC to other time scales. */
174    j = eraUtctai(utc1, utc2, &tai1, &tai2);
175    if ( j < 0 ) return -1;
176    j = eraTaitt(tai1, tai2, &tt1, &tt2);
177    j = eraUtcut1(utc1, utc2, dut1, &ut11, &ut12);
178    if ( j < 0 ) return -1;
179 
180 /* TIO locator s'. */
181    sp = eraSp00(tt1, tt2);
182 
183 /* Earth rotation angle. */
184    theta = eraEra00(ut11, ut12);
185 
186 /* Refraction constants A and B. */
187    eraRefco(phpa, tc, rh, wl, &refa, &refb);
188 
189 /* CIRS <-> observed astrometry parameters. */
190    eraApio(sp, theta, elong, phi, hm, xp, yp, refa, refb, astrom);
191 
192 /* Return any warning status. */
193    return j;
194 
195 /* Finished. */
196 
197 }
198 /*----------------------------------------------------------------------
199 **
200 **
201 **  Copyright (C) 2013-2014, NumFOCUS Foundation.
202 **  All rights reserved.
203 **
204 **  This library is derived, with permission, from the International
205 **  Astronomical Union's "Standards of Fundamental Astronomy" library,
206 **  available from http://www.iausofa.org.
207 **
208 **  The ERFA version is intended to retain identical functionality to
209 **  the SOFA library, but made distinct through different function and
210 **  file names, as set out in the SOFA license conditions.  The SOFA
211 **  original has a role as a reference standard for the IAU and IERS,
212 **  and consequently redistribution is permitted only in its unaltered
213 **  state.  The ERFA version is not subject to this restriction and
214 **  therefore can be included in distributions which do not support the
215 **  concept of "read only" software.
216 **
217 **  Although the intent is to replicate the SOFA API (other than
218 **  replacement of prefix names) and results (with the exception of
219 **  bugs;  any that are discovered will be fixed), SOFA is not
220 **  responsible for any errors found in this version of the library.
221 **
222 **  If you wish to acknowledge the SOFA heritage, please acknowledge
223 **  that you are using a library derived from SOFA, rather than SOFA
224 **  itself.
225 **
226 **
227 **  TERMS AND CONDITIONS
228 **
229 **  Redistribution and use in source and binary forms, with or without
230 **  modification, are permitted provided that the following conditions
231 **  are met:
232 **
233 **  1 Redistributions of source code must retain the above copyright
234 **    notice, this list of conditions and the following disclaimer.
235 **
236 **  2 Redistributions in binary form must reproduce the above copyright
237 **    notice, this list of conditions and the following disclaimer in
238 **    the documentation and/or other materials provided with the
239 **    distribution.
240 **
241 **  3 Neither the name of the Standards Of Fundamental Astronomy Board,
242 **    the International Astronomical Union nor the names of its
243 **    contributors may be used to endorse or promote products derived
244 **    from this software without specific prior written permission.
245 **
246 **  THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
247 **  "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
248 **  LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
249 **  FOR A PARTICULAR PURPOSE ARE DISCLAIMED.  IN NO EVENT SHALL THE
250 **  COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
251 **  INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
252 **  BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
253 **  LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
254 **  CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
255 **  LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
256 **  ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
257 **  POSSIBILITY OF SUCH DAMAGE.
258 **
259 */
260