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#include "erfa.h" |
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int eraApio13(double utc1, double utc2, double dut1, |
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double elong, double phi, double hm, double xp, double yp, |
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double phpa, double tc, double rh, double wl, |
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eraASTROM *astrom) |
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/* |
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** - - - - - - - - - - |
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** e r a A p i o 1 3 |
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** - - - - - - - - - - |
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** |
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** For a terrestrial observer, prepare star-independent astrometry |
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** parameters for transformations between CIRS and observed |
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** coordinates. The caller supplies UTC, site coordinates, ambient air |
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** conditions and observing wavelength. |
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** |
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** Given: |
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** utc1 double UTC as a 2-part... |
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** utc2 double ...quasi Julian Date (Notes 1,2) |
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** dut1 double UT1-UTC (seconds) |
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** elong double longitude (radians, east +ve, Note 3) |
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** phi double geodetic latitude (radians, Note 3) |
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** hm double height above ellipsoid (m, geodetic Notes 4,6) |
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** xp,yp double polar motion coordinates (radians, Note 5) |
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** phpa double pressure at the observer (hPa = mB, Note 6) |
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** tc double ambient temperature at the observer (deg C) |
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** rh double relative humidity at the observer (range 0-1) |
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** wl double wavelength (micrometers, Note 7) |
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** |
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** Returned: |
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** astrom eraASTROM* star-independent astrometry parameters: |
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** pmt double unchanged |
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** eb double[3] unchanged |
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** eh double[3] unchanged |
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** em double unchanged |
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** v double[3] unchanged |
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** bm1 double unchanged |
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** bpn double[3][3] unchanged |
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** along double longitude + s' (radians) |
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** xpl double polar motion xp wrt local meridian (radians) |
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** ypl double polar motion yp wrt local meridian (radians) |
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** sphi double sine of geodetic latitude |
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** cphi double cosine of geodetic latitude |
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** diurab double magnitude of diurnal aberration vector |
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** eral double "local" Earth rotation angle (radians) |
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** refa double refraction constant A (radians) |
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** refb double refraction constant B (radians) |
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** |
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** Returned (function value): |
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** int status: +1 = dubious year (Note 2) |
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** 0 = OK |
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** -1 = unacceptable date |
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** |
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** Notes: |
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** |
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** 1) utc1+utc2 is quasi Julian Date (see Note 2), apportioned in any |
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** convenient way between the two arguments, for example where utc1 |
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** is the Julian Day Number and utc2 is the fraction of a day. |
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** |
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** However, JD cannot unambiguously represent UTC during a leap |
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** second unless special measures are taken. The convention in the |
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** present function is that the JD day represents UTC days whether |
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** the length is 86399, 86400 or 86401 SI seconds. |
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** |
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** Applications should use the function eraDtf2d to convert from |
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** calendar date and time of day into 2-part quasi Julian Date, as |
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** it implements the leap-second-ambiguity convention just |
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** described. |
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** |
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** 2) The warning status "dubious year" flags UTCs that predate the |
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** introduction of the time scale or that are too far in the future |
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** to be trusted. See eraDat for further details. |
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** |
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** 3) UT1-UTC is tabulated in IERS bulletins. It increases by exactly |
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** one second at the end of each positive UTC leap second, |
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** introduced in order to keep UT1-UTC within +/- 0.9s. n.b. This |
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** practice is under review, and in the future UT1-UTC may grow |
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** essentially without limit. |
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** |
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** 4) The geographical coordinates are with respect to the ERFA_WGS84 |
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** reference ellipsoid. TAKE CARE WITH THE LONGITUDE SIGN: the |
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** longitude required by the present function is east-positive |
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** (i.e. right-handed), in accordance with geographical convention. |
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** |
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** 5) The polar motion xp,yp can be obtained from IERS bulletins. The |
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** values are the coordinates (in radians) of the Celestial |
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** Intermediate Pole with respect to the International Terrestrial |
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** Reference System (see IERS Conventions 2003), measured along the |
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** meridians 0 and 90 deg west respectively. For many applications, |
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** xp and yp can be set to zero. |
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** |
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** Internally, the polar motion is stored in a form rotated onto |
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** the local meridian. |
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** |
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** 6) If hm, the height above the ellipsoid of the observing station |
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** in meters, is not known but phpa, the pressure in hPa (=mB), is |
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** available, an adequate estimate of hm can be obtained from the |
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** expression |
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** |
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** hm = -29.3 * tsl * log ( phpa / 1013.25 ); |
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** |
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** where tsl is the approximate sea-level air temperature in K |
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** (See Astrophysical Quantities, C.W.Allen, 3rd edition, section |
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** 52). Similarly, if the pressure phpa is not known, it can be |
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** estimated from the height of the observing station, hm, as |
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** follows: |
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** |
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** phpa = 1013.25 * exp ( -hm / ( 29.3 * tsl ) ); |
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** |
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** Note, however, that the refraction is nearly proportional to the |
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** pressure and that an accurate phpa value is important for |
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** precise work. |
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** |
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** 7) The argument wl specifies the observing wavelength in |
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** micrometers. The transition from optical to radio is assumed to |
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** occur at 100 micrometers (about 3000 GHz). |
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** |
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** 8) It is advisable to take great care with units, as even unlikely |
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** values of the input parameters are accepted and processed in |
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** accordance with the models used. |
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** |
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** 9) In cases where the caller wishes to supply his own Earth |
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** rotation information and refraction constants, the function |
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** eraApc can be used instead of the present function. |
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** |
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** 10) This is one of several functions that inserts into the astrom |
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** structure star-independent parameters needed for the chain of |
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** astrometric transformations ICRS <-> GCRS <-> CIRS <-> observed. |
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** |
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** The various functions support different classes of observer and |
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** portions of the transformation chain: |
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** |
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** functions observer transformation |
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** |
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** eraApcg eraApcg13 geocentric ICRS <-> GCRS |
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** eraApci eraApci13 terrestrial ICRS <-> CIRS |
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** eraApco eraApco13 terrestrial ICRS <-> observed |
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** eraApcs eraApcs13 space ICRS <-> GCRS |
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** eraAper eraAper13 terrestrial update Earth rotation |
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** eraApio eraApio13 terrestrial CIRS <-> observed |
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** |
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** Those with names ending in "13" use contemporary ERFA models to |
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** compute the various ephemerides. The others accept ephemerides |
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** supplied by the caller. |
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** |
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** The transformation from ICRS to GCRS covers space motion, |
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** parallax, light deflection, and aberration. From GCRS to CIRS |
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** comprises frame bias and precession-nutation. From CIRS to |
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** observed takes account of Earth rotation, polar motion, diurnal |
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** aberration and parallax (unless subsumed into the ICRS <-> GCRS |
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** transformation), and atmospheric refraction. |
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** |
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** 11) The context structure astrom produced by this function is used |
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** by eraAtioq and eraAtoiq. |
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** |
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** Called: |
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** eraUtctai UTC to TAI |
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** eraTaitt TAI to TT |
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** eraUtcut1 UTC to UT1 |
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** eraSp00 the TIO locator s', IERS 2000 |
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** eraEra00 Earth rotation angle, IAU 2000 |
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** eraRefco refraction constants for given ambient conditions |
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** eraApio astrometry parameters, CIRS-observed |
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** |
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** Copyright (C) 2013-2019, NumFOCUS Foundation. |
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** Derived, with permission, from the SOFA library. See notes at end of file. |
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*/ |
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{ |
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int j; |
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double tai1, tai2, tt1, tt2, ut11, ut12, sp, theta, refa, refb; |
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/* UTC to other time scales. */ |
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j = eraUtctai(utc1, utc2, &tai1, &tai2); |
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if ( j < 0 ) return -1; |
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j = eraTaitt(tai1, tai2, &tt1, &tt2); |
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j = eraUtcut1(utc1, utc2, dut1, &ut11, &ut12); |
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if ( j < 0 ) return -1; |
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/* TIO locator s'. */ |
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sp = eraSp00(tt1, tt2); |
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/* Earth rotation angle. */ |
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theta = eraEra00(ut11, ut12); |
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/* Refraction constants A and B. */ |
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eraRefco(phpa, tc, rh, wl, &refa, &refb); |
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/* CIRS <-> observed astrometry parameters. */ |
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eraApio(sp, theta, elong, phi, hm, xp, yp, refa, refb, astrom); |
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/* Return any warning status. */ |
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return j; |
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/* Finished. */ |
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} |
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/*---------------------------------------------------------------------- |
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** |
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** |
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** Copyright (C) 2013-2019, NumFOCUS Foundation. |
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** All rights reserved. |
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** |
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** This library is derived, with permission, from the International |
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** Astronomical Union's "Standards of Fundamental Astronomy" library, |
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** available from http://www.iausofa.org. |
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** |
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** The ERFA version is intended to retain identical functionality to |
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** the SOFA library, but made distinct through different function and |
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** file names, as set out in the SOFA license conditions. The SOFA |
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** original has a role as a reference standard for the IAU and IERS, |
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** and consequently redistribution is permitted only in its unaltered |
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** state. The ERFA version is not subject to this restriction and |
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** therefore can be included in distributions which do not support the |
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** concept of "read only" software. |
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** |
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** Although the intent is to replicate the SOFA API (other than |
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** replacement of prefix names) and results (with the exception of |
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** bugs; any that are discovered will be fixed), SOFA is not |
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** responsible for any errors found in this version of the library. |
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** |
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** If you wish to acknowledge the SOFA heritage, please acknowledge |
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** that you are using a library derived from SOFA, rather than SOFA |
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** itself. |
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** |
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** |
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** TERMS AND CONDITIONS |
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** |
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** Redistribution and use in source and binary forms, with or without |
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** modification, are permitted provided that the following conditions |
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** are met: |
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** |
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** 1 Redistributions of source code must retain the above copyright |
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** notice, this list of conditions and the following disclaimer. |
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** |
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** 2 Redistributions in binary form must reproduce the above copyright |
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** notice, this list of conditions and the following disclaimer in |
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** the documentation and/or other materials provided with the |
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** distribution. |
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** |
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** 3 Neither the name of the Standards Of Fundamental Astronomy Board, |
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** the International Astronomical Union nor the names of its |
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** contributors may be used to endorse or promote products derived |
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** from this software without specific prior written permission. |
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** |
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** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS |
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** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT |
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** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS |
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** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE |
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** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, |
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** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, |
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** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; |
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** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER |
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** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT |
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** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN |
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** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE |
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** POSSIBILITY OF SUCH DAMAGE. |
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** |
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*/ |