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Diffstat (limited to 'ast/pal/palRvlsrk.c')
-rw-r--r-- | ast/pal/palRvlsrk.c | 116 |
1 files changed, 116 insertions, 0 deletions
diff --git a/ast/pal/palRvlsrk.c b/ast/pal/palRvlsrk.c new file mode 100644 index 0000000..13bdcef --- /dev/null +++ b/ast/pal/palRvlsrk.c @@ -0,0 +1,116 @@ +/* +*+ +* Name: +* palRvlsrk + +* Purpose: +* Velocity component in a given direction due to the Sun's motion +* with respect to an adopted kinematic Local Standard of Rest. + +* Language: +* Starlink ANSI C + +* Type of Module: +* Library routine + +* Invocation: +* double palRvlsrk( double r2000, double d2000 ) + +* Arguments: +* r2000 = double (Given) +* J2000.0 mean RA (radians) +* d2000 = double (Given) +* J2000.0 mean Dec (radians) + +* Returned Value: +* Component of "standard" solar motion in direction R2000,D2000 (km/s). + +* Description: +* This function returns the velocity component in a given direction +* due to the Sun's motion with respect to an adopted kinematic +* Local Standard of Rest. The result is +ve when the Sun is receding +* from the given point on the sky. + +* Notes: +* - The Local Standard of Rest used here is one of several +* "kinematical" LSRs in common use. A kinematical LSR is the mean +* standard of rest of specified star catalogues or stellar +* populations. The Sun's motion with respect to a kinematical LSR +* is known as the "standard" solar motion. +* - There is another sort of LSR, the "dynamical" LSR, which is a +* point in the vicinity of the Sun which is in a circular orbit +* around the Galactic centre. The Sun's motion with respect to +* the dynamical LSR is called the "peculiar" solar motion. To +* obtain a radial velocity correction with respect to the +* dynamical LSR use the routine sla_RVLSRD. + +* Reference: +* - Delhaye (1965), in "Stars and Stellar Systems", vol 5, p73. + +* Authors: +* PTW: Pat Wallace (STFC) +* DSB: David Berry (JAC, Hawaii) +* {enter_new_authors_here} + +* History: +* 2012-02-16 (DSB): +* Initial version. +* Adapted with permission from the Fortran SLALIB library. +* {enter_further_changes_here} + +* Copyright: +* Copyright (C) 1995 Rutherford Appleton Laboratory +* Copyright (C) 2012 Science and Technology Facilities Council. +* All Rights Reserved. + +* Licence: +* This program is free software: you can redistribute it and/or +* modify it under the terms of the GNU Lesser General Public +* License as published by the Free Software Foundation, either +* version 3 of the License, or (at your option) any later +* version. +* +* This program is distributed in the hope that it will be useful, +* but WITHOUT ANY WARRANTY; without even the implied warranty of +* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the +* GNU Lesser General Public License for more details. +* +* You should have received a copy of the GNU Lesser General +* License along with this program. If not, see +* <http://www.gnu.org/licenses/>. + +* Bugs: +* {note_any_bugs_here} +*- +*/ + +#include "pal.h" +#include "pal1sofa.h" + +double palRvlsrk( double r2000, double d2000 ){ + +/* Local Variables: */ + double vb[ 3 ]; + +/* +* Standard solar motion (from Methods of Experimental Physics, ed Meeks, +* vol 12, part C, sec 6.1.5.2, p281): +* +* 20 km/s towards RA 18h Dec +30d (1900). +* +* The solar motion is expressed here in the form of a J2000.0 +* equatorial Cartesian vector: +* +* VA(1) = X = -SPEED*COS(RA)*COS(DEC) +* VA(2) = Y = -SPEED*SIN(RA)*COS(DEC) +* VA(3) = Z = -SPEED*SIN(DEC) +*/ + + double va[ 3 ] = { -0.29000, +17.31726, -10.00141 }; + +/* Convert given J2000 RA,Dec to x,y,z. */ + eraS2c( r2000, d2000, vb ); + +/* Compute dot product with Solar motion vector. */ + return eraPdp( va, vb ); +} |