| 1 | #include "erfa.h"
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| 2 |
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| 3 | int eraApio13(double utc1, double utc2, double dut1,
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| 4 | double elong, double phi, double hm, double xp, double yp,
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| 5 | double phpa, double tc, double rh, double wl,
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| 6 | eraASTROM *astrom)
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| 7 | /*
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| 8 | ** - - - - - - - - - -
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| 9 | ** e r a A p i o 1 3
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| 10 | ** - - - - - - - - - -
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| 11 | **
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| 12 | ** For a terrestrial observer, prepare star-independent astrometry
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| 13 | ** parameters for transformations between CIRS and observed
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| 14 | ** coordinates. The caller supplies UTC, site coordinates, ambient air
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| 15 | ** conditions and observing wavelength.
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| 16 | **
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| 17 | ** Given:
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| 18 | ** utc1 double UTC as a 2-part...
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| 19 | ** utc2 double ...quasi Julian Date (Notes 1,2)
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| 20 | ** dut1 double UT1-UTC (seconds)
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| 21 | ** elong double longitude (radians, east +ve, Note 3)
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| 22 | ** phi double geodetic latitude (radians, Note 3)
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| 23 | ** hm double height above ellipsoid (m, geodetic Notes 4,6)
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| 24 | ** xp,yp double polar motion coordinates (radians, Note 5)
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| 25 | ** phpa double pressure at the observer (hPa = mB, Note 6)
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| 26 | ** tc double ambient temperature at the observer (deg C)
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| 27 | ** rh double relative humidity at the observer (range 0-1)
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| 28 | ** wl double wavelength (micrometers, Note 7)
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| 29 | **
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| 30 | ** Returned:
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| 31 | ** astrom eraASTROM* star-independent astrometry parameters:
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| 32 | ** pmt double unchanged
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| 33 | ** eb double[3] unchanged
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| 34 | ** eh double[3] unchanged
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| 35 | ** em double unchanged
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| 36 | ** v double[3] unchanged
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| 37 | ** bm1 double unchanged
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| 38 | ** bpn double[3][3] unchanged
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| 39 | ** along double longitude + s' (radians)
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| 40 | ** xpl double polar motion xp wrt local meridian (radians)
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| 41 | ** ypl double polar motion yp wrt local meridian (radians)
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| 42 | ** sphi double sine of geodetic latitude
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| 43 | ** cphi double cosine of geodetic latitude
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| 44 | ** diurab double magnitude of diurnal aberration vector
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| 45 | ** eral double "local" Earth rotation angle (radians)
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| 46 | ** refa double refraction constant A (radians)
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| 47 | ** refb double refraction constant B (radians)
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| 48 | **
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| 49 | ** Returned (function value):
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| 50 | ** int status: +1 = dubious year (Note 2)
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| 51 | ** 0 = OK
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| 52 | ** -1 = unacceptable date
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| 53 | **
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| 54 | ** Notes:
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| 55 | **
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| 56 | ** 1) utc1+utc2 is quasi Julian Date (see Note 2), apportioned in any
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| 57 | ** convenient way between the two arguments, for example where utc1
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| 58 | ** is the Julian Day Number and utc2 is the fraction of a day.
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| 59 | **
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| 60 | ** However, JD cannot unambiguously represent UTC during a leap
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| 61 | ** second unless special measures are taken. The convention in the
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| 62 | ** present function is that the JD day represents UTC days whether
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| 63 | ** the length is 86399, 86400 or 86401 SI seconds.
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| 64 | **
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| 65 | ** Applications should use the function eraDtf2d to convert from
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| 66 | ** calendar date and time of day into 2-part quasi Julian Date, as
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| 67 | ** it implements the leap-second-ambiguity convention just
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| 68 | ** described.
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| 69 | **
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| 70 | ** 2) The warning status "dubious year" flags UTCs that predate the
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| 71 | ** introduction of the time scale or that are too far in the future
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| 72 | ** to be trusted. See eraDat for further details.
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| 73 | **
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| 74 | ** 3) UT1-UTC is tabulated in IERS bulletins. It increases by exactly
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| 75 | ** one second at the end of each positive UTC leap second,
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| 76 | ** introduced in order to keep UT1-UTC within +/- 0.9s. n.b. This
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| 77 | ** practice is under review, and in the future UT1-UTC may grow
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| 78 | ** essentially without limit.
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| 79 | **
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| 80 | ** 4) The geographical coordinates are with respect to the ERFA_WGS84
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| 81 | ** reference ellipsoid. TAKE CARE WITH THE LONGITUDE SIGN: the
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| 82 | ** longitude required by the present function is east-positive
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| 83 | ** (i.e. right-handed), in accordance with geographical convention.
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| 84 | **
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| 85 | ** 5) The polar motion xp,yp can be obtained from IERS bulletins. The
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| 86 | ** values are the coordinates (in radians) of the Celestial
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| 87 | ** Intermediate Pole with respect to the International Terrestrial
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| 88 | ** Reference System (see IERS Conventions 2003), measured along the
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| 89 | ** meridians 0 and 90 deg west respectively. For many applications,
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| 90 | ** xp and yp can be set to zero.
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| 91 | **
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| 92 | ** Internally, the polar motion is stored in a form rotated onto
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| 93 | ** the local meridian.
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| 94 | **
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| 95 | ** 6) If hm, the height above the ellipsoid of the observing station
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| 96 | ** in meters, is not known but phpa, the pressure in hPa (=mB), is
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| 97 | ** available, an adequate estimate of hm can be obtained from the
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| 98 | ** expression
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| 99 | **
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| 100 | ** hm = -29.3 * tsl * log ( phpa / 1013.25 );
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| 101 | **
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| 102 | ** where tsl is the approximate sea-level air temperature in K
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| 103 | ** (See Astrophysical Quantities, C.W.Allen, 3rd edition, section
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| 104 | ** 52). Similarly, if the pressure phpa is not known, it can be
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| 105 | ** estimated from the height of the observing station, hm, as
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| 106 | ** follows:
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| 107 | **
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| 108 | ** phpa = 1013.25 * exp ( -hm / ( 29.3 * tsl ) );
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| 109 | **
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| 110 | ** Note, however, that the refraction is nearly proportional to the
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| 111 | ** pressure and that an accurate phpa value is important for
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| 112 | ** precise work.
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| 113 | **
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| 114 | ** 7) The argument wl specifies the observing wavelength in
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| 115 | ** micrometers. The transition from optical to radio is assumed to
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| 116 | ** occur at 100 micrometers (about 3000 GHz).
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| 117 | **
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| 118 | ** 8) It is advisable to take great care with units, as even unlikely
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| 119 | ** values of the input parameters are accepted and processed in
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| 120 | ** accordance with the models used.
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| 121 | **
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| 122 | ** 9) In cases where the caller wishes to supply his own Earth
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| 123 | ** rotation information and refraction constants, the function
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| 124 | ** eraApc can be used instead of the present function.
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| 125 | **
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| 126 | ** 10) This is one of several functions that inserts into the astrom
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| 127 | ** structure star-independent parameters needed for the chain of
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| 128 | ** astrometric transformations ICRS <-> GCRS <-> CIRS <-> observed.
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| 129 | **
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| 130 | ** The various functions support different classes of observer and
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| 131 | ** portions of the transformation chain:
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| 132 | **
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| 133 | ** functions observer transformation
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| 134 | **
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| 135 | ** eraApcg eraApcg13 geocentric ICRS <-> GCRS
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| 136 | ** eraApci eraApci13 terrestrial ICRS <-> CIRS
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| 137 | ** eraApco eraApco13 terrestrial ICRS <-> observed
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| 138 | ** eraApcs eraApcs13 space ICRS <-> GCRS
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| 139 | ** eraAper eraAper13 terrestrial update Earth rotation
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| 140 | ** eraApio eraApio13 terrestrial CIRS <-> observed
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| 141 | **
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| 142 | ** Those with names ending in "13" use contemporary ERFA models to
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| 143 | ** compute the various ephemerides. The others accept ephemerides
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| 144 | ** supplied by the caller.
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| 145 | **
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| 146 | ** The transformation from ICRS to GCRS covers space motion,
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| 147 | ** parallax, light deflection, and aberration. From GCRS to CIRS
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| 148 | ** comprises frame bias and precession-nutation. From CIRS to
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| 149 | ** observed takes account of Earth rotation, polar motion, diurnal
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| 150 | ** aberration and parallax (unless subsumed into the ICRS <-> GCRS
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| 151 | ** transformation), and atmospheric refraction.
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| 152 | **
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| 153 | ** 11) The context structure astrom produced by this function is used
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| 154 | ** by eraAtioq and eraAtoiq.
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| 155 | **
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| 156 | ** Called:
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| 157 | ** eraUtctai UTC to TAI
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| 158 | ** eraTaitt TAI to TT
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| 159 | ** eraUtcut1 UTC to UT1
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| 160 | ** eraSp00 the TIO locator s', IERS 2000
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| 161 | ** eraEra00 Earth rotation angle, IAU 2000
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| 162 | ** eraRefco refraction constants for given ambient conditions
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| 163 | ** eraApio astrometry parameters, CIRS-observed
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| 164 | **
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| 165 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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| 166 | ** Derived, with permission, from the SOFA library. See notes at end of file.
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| 167 | */
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| 168 | {
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| 169 | int j;
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| 170 | double tai1, tai2, tt1, tt2, ut11, ut12, sp, theta, refa, refb;
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| 171 |
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| 172 |
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| 173 | /* UTC to other time scales. */
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| 174 | j = eraUtctai(utc1, utc2, &tai1, &tai2);
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| 175 | if ( j < 0 ) return -1;
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| 176 | j = eraTaitt(tai1, tai2, &tt1, &tt2);
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| 177 | j = eraUtcut1(utc1, utc2, dut1, &ut11, &ut12);
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| 178 | if ( j < 0 ) return -1;
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| 179 |
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| 180 | /* TIO locator s'. */
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| 181 | sp = eraSp00(tt1, tt2);
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| 182 |
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| 183 | /* Earth rotation angle. */
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| 184 | theta = eraEra00(ut11, ut12);
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| 185 |
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| 186 | /* Refraction constants A and B. */
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| 187 | eraRefco(phpa, tc, rh, wl, &refa, &refb);
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| 188 |
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| 189 | /* CIRS <-> observed astrometry parameters. */
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| 190 | eraApio(sp, theta, elong, phi, hm, xp, yp, refa, refb, astrom);
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| 191 |
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| 192 | /* Return any warning status. */
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| 193 | return j;
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| 194 |
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| 195 | /* Finished. */
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| 196 |
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| 197 | }
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| 198 | /*----------------------------------------------------------------------
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| 199 | **
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| 200 | **
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| 201 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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| 202 | ** All rights reserved.
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| 203 | **
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| 204 | ** This library is derived, with permission, from the International
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| 205 | ** Astronomical Union's "Standards of Fundamental Astronomy" library,
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| 206 | ** available from http://www.iausofa.org.
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| 207 | **
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| 208 | ** The ERFA version is intended to retain identical functionality to
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| 209 | ** the SOFA library, but made distinct through different function and
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| 210 | ** file names, as set out in the SOFA license conditions. The SOFA
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| 211 | ** original has a role as a reference standard for the IAU and IERS,
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| 212 | ** and consequently redistribution is permitted only in its unaltered
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| 213 | ** state. The ERFA version is not subject to this restriction and
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| 214 | ** therefore can be included in distributions which do not support the
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| 215 | ** concept of "read only" software.
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| 216 | **
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| 217 | ** Although the intent is to replicate the SOFA API (other than
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| 218 | ** replacement of prefix names) and results (with the exception of
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| 219 | ** bugs; any that are discovered will be fixed), SOFA is not
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| 220 | ** responsible for any errors found in this version of the library.
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| 221 | **
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| 222 | ** If you wish to acknowledge the SOFA heritage, please acknowledge
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| 223 | ** that you are using a library derived from SOFA, rather than SOFA
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| 224 | ** itself.
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| 225 | **
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| 226 | **
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| 227 | ** TERMS AND CONDITIONS
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| 228 | **
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| 229 | ** Redistribution and use in source and binary forms, with or without
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| 230 | ** modification, are permitted provided that the following conditions
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| 231 | ** are met:
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| 232 | **
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| 233 | ** 1 Redistributions of source code must retain the above copyright
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| 234 | ** notice, this list of conditions and the following disclaimer.
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| 235 | **
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| 236 | ** 2 Redistributions in binary form must reproduce the above copyright
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| 237 | ** notice, this list of conditions and the following disclaimer in
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| 238 | ** the documentation and/or other materials provided with the
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| 239 | ** distribution.
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| 240 | **
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| 241 | ** 3 Neither the name of the Standards Of Fundamental Astronomy Board,
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| 242 | ** the International Astronomical Union nor the names of its
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| 243 | ** contributors may be used to endorse or promote products derived
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| 244 | ** from this software without specific prior written permission.
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| 245 | **
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| 246 | ** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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| 247 | ** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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| 248 | ** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
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| 249 | ** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
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| 250 | ** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
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| 251 | ** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
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| 252 | ** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
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| 253 | ** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
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| 254 | ** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
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| 255 | ** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
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| 256 | ** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
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| 257 | ** POSSIBILITY OF SUCH DAMAGE.
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| 258 | **
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| 259 | */
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