File Coverage

erfasrc/src/atoc13.c
Criterion Covered Total %
statement 0 6 0.0
branch 0 2 0.0
condition n/a
subroutine n/a
pod n/a
total 0 8 0.0


line stmt bran cond sub pod time code
1             #include "erfa.h"
2              
3 0           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) 2013-2019, 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 0           j = eraApco13(utc1, utc2, dut1, elong, phi, hm, xp, yp,
155             phpa, tc, rh, wl, &astrom, &eo);
156              
157             /* Abort if bad UTC. */
158 0 0         if ( j < 0 ) return j;
159              
160             /* Transform observed to CIRS. */
161 0           eraAtoiq(type, ob1, ob2, &astrom, &ri, &di);
162              
163             /* Transform CIRS to ICRS. */
164 0           eraAticq(ri, di, &astrom, rc, dc);
165              
166             /* Return OK/warning status. */
167 0           return j;
168              
169             /* Finished. */
170              
171             }
172             /*----------------------------------------------------------------------
173             **
174             **
175             ** Copyright (C) 2013-2019, 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             */