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/* |
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*+ |
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* Name: |
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* palPlantu |
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* Purpose: |
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* Topocentric RA,Dec of a Solar-System object from universal elements |
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* Language: |
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* Starlink ANSI C |
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* Type of Module: |
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* Library routine |
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* Invocation: |
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* void palPlantu ( double date, double elong, double phi, const double u[13], |
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* double *ra, double *dec, double *r, int *jstat ) { |
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* Description: |
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* Topocentric apparent RA,Dec of a Solar-System object whose |
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* heliocentric universal elements are known. |
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* Arguments: |
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* date = double (Given) |
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* TT MJD of observation (JD-2400000.5) |
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* elong = double (Given) |
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* Observer's east longitude (radians) |
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* phi = double (Given) |
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* Observer's geodetic latitude (radians) |
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* u = const double [13] (Given) |
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* Universal orbital elements |
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* - (0) combined mass (M+m) |
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* - (1) total energy of the orbit (alpha) |
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* - (2) reference (osculating) epoch (t0) |
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* - (3-5) position at reference epoch (r0) |
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* - (6-8) velocity at reference epoch (v0) |
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* - (9) heliocentric distance at reference epoch |
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* - (10) r0.v0 |
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* - (11) date (t) |
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* - (12) universal eccentric anomaly (psi) of date, approx |
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* ra = double * (Returned) |
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* Topocentric apparent RA (radians) |
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* dec = double * (Returned) |
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* Topocentric apparent Dec (radians) |
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* r = double * (Returned) |
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* Distance from observer (AU) |
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* jstat = int * (Returned) |
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* status: 0 = OK |
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* - -1 = radius vector zero |
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* - -2 = failed to converge |
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* Authors: |
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* PTW: Pat Wallace (STFC) |
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* TIMJ: Tim Jenness (JAC, Hawaii) |
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* {enter_new_authors_here} |
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* Notes: |
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* - DATE is the instant for which the prediction is required. It is |
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* in the TT timescale (formerly Ephemeris Time, ET) and is a |
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* Modified Julian Date (JD-2400000.5). |
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* - The longitude and latitude allow correction for geocentric |
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* parallax. This is usually a small effect, but can become |
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* important for near-Earth asteroids. Geocentric positions can be |
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* generated by appropriate use of routines palEpv (or palEvp) and |
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* palUe2pv. |
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* - The "universal" elements are those which define the orbit for the |
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* purposes of the method of universal variables (see reference 2). |
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* They consist of the combined mass of the two bodies, an epoch, |
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* and the position and velocity vectors (arbitrary reference frame) |
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* at that epoch. The parameter set used here includes also various |
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* quantities that can, in fact, be derived from the other |
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* information. This approach is taken to avoiding unnecessary |
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* computation and loss of accuracy. The supplementary quantities |
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* are (i) alpha, which is proportional to the total energy of the |
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* orbit, (ii) the heliocentric distance at epoch, (iii) the |
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* outwards component of the velocity at the given epoch, (iv) an |
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* estimate of psi, the "universal eccentric anomaly" at a given |
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* date and (v) that date. |
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* - The universal elements are with respect to the J2000 equator and |
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* equinox. |
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82
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* See Also: |
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* - Sterne, Theodore E., "An Introduction to Celestial Mechanics", |
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* Interscience Publishers Inc., 1960. Section 6.7, p199. |
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* - Everhart, E. & Pitkin, E.T., Am.J.Phys. 51, 712, 1983. |
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* History: |
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* 2012-03-12 (TIMJ): |
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* Initial version direct conversion of SLA/F. |
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* Adapted with permission from the Fortran SLALIB library. |
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* {enter_further_changes_here} |
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* Copyright: |
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* Copyright (C) 2005 Patrick T. Wallace |
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* Copyright (C) 2012 Science and Technology Facilities Council. |
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* All Rights Reserved. |
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* Licence: |
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* This program is free software; you can redistribute it and/or |
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* modify it under the terms of the GNU General Public License as |
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* published by the Free Software Foundation; either version 3 of |
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* the License, or (at your option) any later version. |
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* |
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* This program is distributed in the hope that it will be |
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* useful, but WITHOUT ANY WARRANTY; without even the implied |
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* warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR |
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* PURPOSE. See the GNU General Public License for more details. |
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* |
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* You should have received a copy of the GNU General Public License |
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* along with this program; if not, write to the Free Software |
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* Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, |
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* MA 02110-1301, USA. |
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114
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* Bugs: |
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* {note_any_bugs_here} |
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*- |
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*/ |
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119
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#include |
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121
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#include "pal.h" |
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#include "palmac.h" |
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124
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#include "pal1sofa.h" |
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126
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1
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void palPlantu ( double date, double elong, double phi, const double u[13], |
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double *ra, double *dec, double *r, int *jstat ) { |
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129
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int i; |
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double dvb[3], dpb[3], vsg[6], vsp[6], v[6], rmat[3][3], |
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vgp[6], stl, vgo[6], dx, dy, dz, d, tl; |
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133
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double ucp[13]; |
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135
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/* To retain the stated const API and conform to the documentation |
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we must copy the contents of the u array as palUe2pv updates |
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the final two elements */ |
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14
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for (i=0;i<13;i++) { |
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13
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ucp[i] = u[i]; |
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} |
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142
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/* Sun to geocentre (J2000, velocity in AU/s) */ |
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1
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palEpv( date, vsg, &(vsg[3]), dpb, dvb ); |
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4
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100
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for (i=3; i < 6; i++) { |
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3
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vsg[i] /= PAL__SPD; |
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} |
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148
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/* Sun to planet (J2000) */ |
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1
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palUe2pv( date, ucp, vsp, jstat ); |
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151
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/* Geocentre to planet (J2000) */ |
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7
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for (i=0; i<6; i++) { |
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6
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v[i] = vsp[i] - vsg[i]; |
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} |
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156
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/* Precession and nutation to date */ |
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1
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palPrenut( 2000.0, date, rmat ); |
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1
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eraRxp(rmat, v, vgp); |
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1
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eraRxp( rmat, &(v[3]), &(vgp[3]) ); |
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161
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/* Geocentre to observer (date) */ |
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1
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stl = palGmst( date - palDt( palEpj(date) ) / PAL__SPD ) + elong; |
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1
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palPvobs( phi, 0.0, stl, vgo ); |
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165
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/* Observer to planet (date) */ |
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7
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for (i=0; i<6; i++) { |
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6
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v[i] = vgp[i] - vgo[i]; |
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} |
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170
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/* Geometric distance (AU) */ |
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1
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dx = v[0]; |
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1
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dy = v[1]; |
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1
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dz = v[2]; |
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1
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d = sqrt( dx*dx + dy*dy + dz*dz ); |
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176
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/* Light time (sec) */ |
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1
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tl = PAL__CR * d; |
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179
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/* Correct position for planetary aberration */ |
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4
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for (i=0; i<3; i++) { |
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3
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v[i] -= tl * v[i+3]; |
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} |
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184
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/* To RA,Dec */ |
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1
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eraC2s( v, ra, dec ); |
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1
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*ra = eraAnp( *ra ); |
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1
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*r = d; |
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1
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} |
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