line |
stmt |
bran |
cond |
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pod |
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#include "erfa.h" |
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void eraAtoiq(const char *type, |
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double ob1, double ob2, eraASTROM *astrom, |
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double *ri, double *di) |
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/* |
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** - - - - - - - - - |
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** e r a A t o i q |
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** - - - - - - - - - |
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** |
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** Quick observed place to CIRS, given the star-independent astrometry |
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** parameters. |
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** |
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** Use of this function is appropriate when efficiency is important and |
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** where many star positions are all to be transformed for one date. |
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** The star-independent astrometry parameters can be obtained by |
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** calling eraApio[13] or eraApco[13]. |
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** |
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** Given: |
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** type char[] type of coordinates: "R", "H" or "A" (Note 1) |
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** ob1 double observed Az, HA or RA (radians; Az is N=0,E=90) |
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** ob2 double observed ZD or Dec (radians) |
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** astrom eraASTROM* star-independent astrometry parameters: |
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** pmt double PM time interval (SSB, Julian years) |
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** eb double[3] SSB to observer (vector, au) |
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** eh double[3] Sun to observer (unit vector) |
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** em double distance from Sun to observer (au) |
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** v double[3] barycentric observer velocity (vector, c) |
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** bm1 double sqrt(1-|v|^2): reciprocal of Lorenz factor |
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** bpn double[3][3] bias-precession-nutation matrix |
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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: |
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** ri double* CIRS right ascension (CIO-based, radians) |
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** di double* CIRS declination (radians) |
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** |
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** Notes: |
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** |
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** 1) "Observed" Az,El means the position that would be seen by a |
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** perfect geodetically aligned theodolite. This is related to |
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** the observed HA,Dec via the standard rotation, using the geodetic |
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** latitude (corrected for polar motion), while the observed HA and |
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** RA are related simply through the Earth rotation angle and the |
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** site longitude. "Observed" RA,Dec or HA,Dec thus means the |
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** position that would be seen by a perfect equatorial with its |
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** polar axis aligned to the Earth's axis of rotation. By removing |
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** from the observed place the effects of atmospheric refraction and |
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** diurnal aberration, the CIRS RA,Dec is obtained. |
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** |
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** 2) Only the first character of the type argument is significant. |
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** "R" or "r" indicates that ob1 and ob2 are the observed right |
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** ascension and declination; "H" or "h" indicates that they are |
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** hour angle (west +ve) and declination; anything else ("A" or |
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** "a" is recommended) indicates that ob1 and ob2 are azimuth (north |
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** zero, east 90 deg) and zenith distance. (Zenith distance is used |
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** rather than altitude in order to reflect the fact that no |
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** allowance is made for depression of the horizon.) |
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** |
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** 3) The accuracy of the result is limited by the corrections for |
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** refraction, which use a simple A*tan(z) + B*tan^3(z) model. |
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** Providing the meteorological parameters are known accurately and |
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** there are no gross local effects, the predicted observed |
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** coordinates should be within 0.05 arcsec (optical) or 1 arcsec |
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** (radio) for a zenith distance of less than 70 degrees, better |
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** than 30 arcsec (optical or radio) at 85 degrees and better than |
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** 20 arcmin (optical) or 30 arcmin (radio) at the horizon. |
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** |
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** Without refraction, the complementary functions eraAtioq and |
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** eraAtoiq are self-consistent to better than 1 microarcsecond all |
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** over the celestial sphere. With refraction included, consistency |
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** falls off at high zenith distances, but is still better than |
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** 0.05 arcsec at 85 degrees. |
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** |
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** 4) 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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** Called: |
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** eraS2c spherical coordinates to unit vector |
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** eraC2s p-vector to spherical |
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** eraAnp normalize angle into range 0 to 2pi |
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** |
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** Copyright (C) 2013-2020, 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 c; |
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double c1, c2, sphi, cphi, ce, xaeo, yaeo, zaeo, v[3], |
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xmhdo, ymhdo, zmhdo, az, sz, zdo, refa, refb, tz, dref, |
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zdt, xaet, yaet, zaet, xmhda, ymhda, zmhda, |
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f, xhd, yhd, zhd, xpl, ypl, w, hma; |
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/* Coordinate type. */ |
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c = (int) type[0]; |
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/* Coordinates. */ |
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c1 = ob1; |
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c2 = ob2; |
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/* Sin, cos of latitude. */ |
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sphi = astrom->sphi; |
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cphi = astrom->cphi; |
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113
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/* Standardize coordinate type. */ |
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if ( c == 'r' || c == 'R' ) { |
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c = 'R'; |
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} else if ( c == 'h' || c == 'H' ) { |
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c = 'H'; |
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} else { |
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c = 'A'; |
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} |
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122
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/* If Az,ZD, convert to Cartesian (S=0,E=90). */ |
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if ( c == 'A' ) { |
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ce = sin(c2); |
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xaeo = - cos(c1) * ce; |
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yaeo = sin(c1) * ce; |
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zaeo = cos(c2); |
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} else { |
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131
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/* If RA,Dec, convert to HA,Dec. */ |
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if ( c == 'R' ) c1 = astrom->eral - c1; |
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134
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/* To Cartesian -HA,Dec. */ |
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eraS2c ( -c1, c2, v ); |
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xmhdo = v[0]; |
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ymhdo = v[1]; |
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zmhdo = v[2]; |
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140
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/* To Cartesian Az,El (S=0,E=90). */ |
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xaeo = sphi*xmhdo - cphi*zmhdo; |
142
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yaeo = ymhdo; |
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zaeo = cphi*xmhdo + sphi*zmhdo; |
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} |
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146
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/* Azimuth (S=0,E=90). */ |
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az = ( xaeo != 0.0 || yaeo != 0.0 ) ? atan2(yaeo,xaeo) : 0.0; |
148
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149
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/* Sine of observed ZD, and observed ZD. */ |
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sz = sqrt ( xaeo*xaeo + yaeo*yaeo ); |
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zdo = atan2 ( sz, zaeo ); |
152
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153
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/* |
154
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** Refraction |
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** ---------- |
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*/ |
157
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158
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/* Fast algorithm using two constant model. */ |
159
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0
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refa = astrom->refa; |
160
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0
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refb = astrom->refb; |
161
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tz = sz / zaeo; |
162
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0
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dref = ( refa + refb*tz*tz ) * tz; |
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zdt = zdo + dref; |
164
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165
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/* To Cartesian Az,ZD. */ |
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ce = sin(zdt); |
167
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xaet = cos(az) * ce; |
168
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0
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yaet = sin(az) * ce; |
169
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zaet = cos(zdt); |
170
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171
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/* Cartesian Az,ZD to Cartesian -HA,Dec. */ |
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xmhda = sphi*xaet + cphi*zaet; |
173
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ymhda = yaet; |
174
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0
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zmhda = - cphi*xaet + sphi*zaet; |
175
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176
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/* Diurnal aberration. */ |
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0
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f = ( 1.0 + astrom->diurab*ymhda ); |
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xhd = f * xmhda; |
179
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0
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yhd = f * ( ymhda - astrom->diurab ); |
180
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zhd = f * zmhda; |
181
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182
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/* Polar motion. */ |
183
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0
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xpl = astrom->xpl; |
184
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0
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ypl = astrom->ypl; |
185
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0
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w = xpl*xhd - ypl*yhd + zhd; |
186
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0
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v[0] = xhd - xpl*w; |
187
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0
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v[1] = yhd + ypl*w; |
188
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0
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v[2] = w - ( xpl*xpl + ypl*ypl ) * zhd; |
189
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190
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/* To spherical -HA,Dec. */ |
191
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0
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eraC2s(v, &hma, di); |
192
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193
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/* Right ascension. */ |
194
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0
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*ri = eraAnp(astrom->eral + hma); |
195
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196
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/* Finished. */ |
197
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198
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0
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} |
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/*---------------------------------------------------------------------- |
200
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** |
201
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** |
202
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** Copyright (C) 2013-2020, NumFOCUS Foundation. |
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** All rights reserved. |
204
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** |
205
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** This library is derived, with permission, from the International |
206
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** Astronomical Union's "Standards of Fundamental Astronomy" library, |
207
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** available from http://www.iausofa.org. |
208
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** |
209
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** The ERFA version is intended to retain identical functionality to |
210
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** the SOFA library, but made distinct through different function and |
211
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** file names, as set out in the SOFA license conditions. The SOFA |
212
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** original has a role as a reference standard for the IAU and IERS, |
213
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** and consequently redistribution is permitted only in its unaltered |
214
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** state. The ERFA version is not subject to this restriction and |
215
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** therefore can be included in distributions which do not support the |
216
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** concept of "read only" software. |
217
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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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*/ |