#include "erfa.h"
void eraAtioq(double ri, double di, eraASTROM *astrom,
double *aob, double *zob,
double *hob, double *dob, double *rob)
/*
** - - - - - - - - -
** e r a A t i o q
** - - - - - - - - -
**
** Quick CIRS to observed place transformation.
**
** Use of this function is appropriate when efficiency is important and
** where many star positions are all to be transformed for one date.
** The star-independent astrometry parameters can be obtained by
** calling eraApio[13] or eraApco[13].
**
** Given:
** ri double CIRS right ascension
** di double CIRS declination
** astrom eraASTROM* star-independent astrometry parameters:
** pmt double PM time interval (SSB, Julian years)
** eb double[3] SSB to observer (vector, au)
** eh double[3] Sun to observer (unit vector)
** em double distance from Sun to observer (au)
** v double[3] barycentric observer velocity (vector, c)
** bm1 double sqrt(1-|v|^2): reciprocal of Lorenz factor
** bpn double[3][3] bias-precession-nutation matrix
** along double longitude + s' (radians)
** xpl double polar motion xp wrt local meridian (radians)
** ypl double polar motion yp wrt local meridian (radians)
** sphi double sine of geodetic latitude
** cphi double cosine of geodetic latitude
** diurab double magnitude of diurnal aberration vector
** eral double "local" Earth rotation angle (radians)
** refa double refraction constant A (radians)
** refb double refraction constant B (radians)
**
** Returned:
** aob double* observed azimuth (radians: N=0,E=90)
** zob double* observed zenith distance (radians)
** hob double* observed hour angle (radians)
** dob double* observed declination (radians)
** rob double* observed right ascension (CIO-based, radians)
**
** Notes:
**
** 1) This function returns zenith distance rather than altitude in
** order to reflect the fact that no allowance is made for
** depression of the horizon.
**
** 2) The accuracy of the result is limited by the corrections for
** refraction, which use a simple A*tan(z) + B*tan^3(z) model.
** Providing the meteorological parameters are known accurately and
** there are no gross local effects, the predicted observed
** coordinates should be within 0.05 arcsec (optical) or 1 arcsec
** (radio) for a zenith distance of less than 70 degrees, better
** than 30 arcsec (optical or radio) at 85 degrees and better
** than 20 arcmin (optical) or 30 arcmin (radio) at the horizon.
**
** Without refraction, the complementary functions eraAtioq and
** eraAtoiq are self-consistent to better than 1 microarcsecond all
** over the celestial sphere. With refraction included, consistency
** falls off at high zenith distances, but is still better than
** 0.05 arcsec at 85 degrees.
**
** 3) It is advisable to take great care with units, as even unlikely
** values of the input parameters are accepted and processed in
** accordance with the models used.
**
** 4) The CIRS RA,Dec is obtained from a star catalog mean place by
** allowing for space motion, parallax, the Sun's gravitational lens
** effect, annual aberration and precession-nutation. For star
** positions in the ICRS, these effects can be applied by means of
** the eraAtci13 (etc.) functions. Starting from classical "mean
** place" systems, additional transformations will be needed first.
**
** 5) "Observed" Az,El means the position that would be seen by a
** perfect geodetically aligned theodolite. This is obtained from
** the CIRS RA,Dec by allowing for Earth orientation and diurnal
** aberration, rotating from equator to horizon coordinates, and
** then adjusting for refraction. The HA,Dec is obtained by
** rotating back into equatorial coordinates, and is the position
** that would be seen by a perfect equatorial with its polar axis
** aligned to the Earth's axis of rotation. Finally, the RA is
** obtained by subtracting the HA from the local ERA.
**
** 6) The star-independent CIRS-to-observed-place parameters in ASTROM
** may be computed with eraApio[13] or eraApco[13]. If nothing has
** changed significantly except the time, eraAper[13] may be used to
** perform the requisite adjustment to the astrom structure.
**
** Called:
** eraS2c spherical coordinates to unit vector
** eraC2s p-vector to spherical
** eraAnp normalize angle into range 0 to 2pi
**
** Copyright (C) 2013-2014, NumFOCUS Foundation.
** Derived, with permission, from the SOFA library. See notes at end of file.
*/
{
/* Minimum cos(alt) and sin(alt) for refraction purposes */
const double CELMIN = 1e-6;
const double SELMIN = 0.05;
double v[3], x, y, z, xhd, yhd, zhd, f, xhdt, yhdt, zhdt,
xaet, yaet, zaet, azobs, r, tz, w, del, cosdel,
xaeo, yaeo, zaeo, zdobs, hmobs, dcobs, raobs;
/*--------------------------------------------------------------------*/
/* CIRS RA,Dec to Cartesian -HA,Dec. */
eraS2c(ri-astrom->eral, di, v);
x = v[0];
y = v[1];
z = v[2];
/* Polar motion. */
xhd = x + astrom->xpl*z;
yhd = y - astrom->ypl*z;
zhd = z - astrom->xpl*x + astrom->ypl*y;
/* Diurnal aberration. */
f = ( 1.0 - astrom->diurab*yhd );
xhdt = f * xhd;
yhdt = f * ( yhd + astrom->diurab );
zhdt = f * zhd;
/* Cartesian -HA,Dec to Cartesian Az,El (S=0,E=90). */
xaet = astrom->sphi*xhdt - astrom->cphi*zhdt;
yaet = yhdt;
zaet = astrom->cphi*xhdt + astrom->sphi*zhdt;
/* Azimuth (N=0,E=90). */
azobs = ( xaet != 0.0 || yaet != 0.0 ) ? atan2(yaet,-xaet) : 0.0;
/* ---------- */
/* Refraction */
/* ---------- */
/* Cosine and sine of altitude, with precautions. */
r = sqrt(xaet*xaet + yaet*yaet);
r = r > CELMIN ? r : CELMIN;
z = zaet > SELMIN ? zaet : SELMIN;
/* A*tan(z)+B*tan^3(z) model, with Newton-Raphson correction. */
tz = r/z;
w = astrom->refb*tz*tz;
del = ( astrom->refa + w ) * tz /
( 1.0 + ( astrom->refa + 3.0*w ) / ( z*z ) );
/* Apply the change, giving observed vector. */
cosdel = 1.0 - del*del/2.0;
f = cosdel - del*z/r;
xaeo = xaet*f;
yaeo = yaet*f;
zaeo = cosdel*zaet + del*r;
/* Observed ZD. */
zdobs = atan2(sqrt(xaeo*xaeo+yaeo*yaeo), zaeo);
/* Az/El vector to HA,Dec vector (both right-handed). */
v[0] = astrom->sphi*xaeo + astrom->cphi*zaeo;
v[1] = yaeo;
v[2] = - astrom->cphi*xaeo + astrom->sphi*zaeo;
/* To spherical -HA,Dec. */
eraC2s ( v, &hmobs, &dcobs );
/* Right ascension (with respect to CIO). */
raobs = astrom->eral + hmobs;
/* Return the results. */
*aob = eraAnp(azobs);
*zob = zdobs;
*hob = -hmobs;
*dob = dcobs;
*rob = eraAnp(raobs);
/* Finished. */
}
/*----------------------------------------------------------------------
**
**
** Copyright (C) 2013-2014, NumFOCUS Foundation.
** All rights reserved.
**
** This library is derived, with permission, from the International
** Astronomical Union's "Standards of Fundamental Astronomy" library,
** available from http://www.iausofa.org.
**
** The ERFA version is intended to retain identical functionality to
** the SOFA library, but made distinct through different function and
** file names, as set out in the SOFA license conditions. The SOFA
** original has a role as a reference standard for the IAU and IERS,
** and consequently redistribution is permitted only in its unaltered
** state. The ERFA version is not subject to this restriction and
** therefore can be included in distributions which do not support the
** concept of "read only" software.
**
** Although the intent is to replicate the SOFA API (other than
** replacement of prefix names) and results (with the exception of
** bugs; any that are discovered will be fixed), SOFA is not
** responsible for any errors found in this version of the library.
**
** If you wish to acknowledge the SOFA heritage, please acknowledge
** that you are using a library derived from SOFA, rather than SOFA
** itself.
**
**
** TERMS AND CONDITIONS
**
** Redistribution and use in source and binary forms, with or without
** modification, are permitted provided that the following conditions
** are met:
**
** 1 Redistributions of source code must retain the above copyright
** notice, this list of conditions and the following disclaimer.
**
** 2 Redistributions in binary form must reproduce the above copyright
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** distribution.
**
** 3 Neither the name of the Standards Of Fundamental Astronomy Board,
** the International Astronomical Union nor the names of its
** contributors may be used to endorse or promote products derived
** from this software without specific prior written permission.
**
** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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*/