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author | Joe Hunkeler <jhunkeler@gmail.com> | 2015-08-11 16:51:37 -0400 |
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committer | Joe Hunkeler <jhunkeler@gmail.com> | 2015-08-11 16:51:37 -0400 |
commit | 40e5a5811c6ffce9b0974e93cdd927cbcf60c157 (patch) | |
tree | 4464880c571602d54f6ae114729bf62a89518057 /math/slalib/mapqk.f | |
download | iraf-osx-40e5a5811c6ffce9b0974e93cdd927cbcf60c157.tar.gz |
Repatch (from linux) of OSX IRAF
Diffstat (limited to 'math/slalib/mapqk.f')
-rw-r--r-- | math/slalib/mapqk.f | 160 |
1 files changed, 160 insertions, 0 deletions
diff --git a/math/slalib/mapqk.f b/math/slalib/mapqk.f new file mode 100644 index 00000000..0e1997ff --- /dev/null +++ b/math/slalib/mapqk.f @@ -0,0 +1,160 @@ + SUBROUTINE slMAPQ (RM, DM, PR, PD, PX, RV, AMPRMS, RA, DA) +*+ +* - - - - - - +* M A P Q +* - - - - - - +* +* Quick mean to apparent place: transform a star RA,Dec from +* mean place to geocentric apparent place, given the +* star-independent parameters. +* +* Use of this routine is appropriate when efficiency is important +* and where many star positions, all referred to the same equator +* and equinox, are to be transformed for one epoch. The +* star-independent parameters can be obtained by calling the +* slMAPA routine. +* +* If the parallax and proper motions are zero the slMAPZ +* routine can be used instead. +* +* The reference frames and timescales used are post IAU 1976. +* +* Given: +* RM,DM d mean RA,Dec (rad) +* PR,PD d proper motions: RA,Dec changes per Julian year +* PX d parallax (arcsec) +* RV d radial velocity (km/sec, +ve if receding) +* +* AMPRMS d(21) star-independent mean-to-apparent parameters: +* +* (1) time interval for proper motion (Julian years) +* (2-4) barycentric position of the Earth (AU) +* (5-7) heliocentric direction of the Earth (unit vector) +* (8) (grav rad Sun)*2/(Sun-Earth distance) +* (9-11) barycentric Earth velocity in units of c +* (12) sqrt(1-v**2) where v=modulus(ABV) +* (13-21) precession/nutation (3,3) matrix +* +* Returned: +* RA,DA d apparent RA,Dec (rad) +* +* References: +* 1984 Astronomical Almanac, pp B39-B41. +* (also Lederle & Schwan, Astron. Astrophys. 134, +* 1-6, 1984) +* +* Notes: +* +* 1) The vectors AMPRMS(2-4) and AMPRMS(5-7) are referred to +* the mean equinox and equator of epoch EQ. +* +* 2) Strictly speaking, the routine is not valid for solar-system +* sources, though the error will usually be extremely small. +* However, to prevent gross errors in the case where the +* position of the Sun is specified, the gravitational +* deflection term is restrained within about 920 arcsec of the +* centre of the Sun's disc. The term has a maximum value of +* about 1.85 arcsec at this radius, and decreases to zero as +* the centre of the disc is approached. +* +* Called: +* slDS2C spherical to Cartesian +* slDVDV dot product +* slDMXV matrix x vector +* slDC2S Cartesian to spherical +* slDA2P normalize angle 0-2Pi +* +* P.T.Wallace Starlink 15 January 2000 +* +* Copyright (C) 2000 Rutherford Appleton Laboratory +* +* License: +* This program is free software; you can redistribute it and/or modify +* it under the terms of the GNU General Public License as published by +* the Free Software Foundation; either version 2 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 General Public License for more details. +* +* You should have received a copy of the GNU General Public License +* along with this program (see SLA_CONDITIONS); if not, write to the +* Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, +* Boston, MA 02110-1301 USA +* +* Copyright (C) 1995 Association of Universities for Research in Astronomy Inc. +*- + + IMPLICIT NONE + + DOUBLE PRECISION RM,DM,PR,PD,PX,RV,AMPRMS(21),RA,DA + +* Arc seconds to radians + DOUBLE PRECISION AS2R + PARAMETER (AS2R=0.484813681109535994D-5) + +* Km/s to AU/year + DOUBLE PRECISION VF + PARAMETER (VF=0.21094502D0) + + INTEGER I + + DOUBLE PRECISION PMT,GR2E,AB1,EB(3),EHN(3),ABV(3), + : Q(3),PXR,W,EM(3),P(3),PN(3),PDE,PDEP1, + : P1(3),P1DV,P2(3),P3(3) + + DOUBLE PRECISION slDVDV,slDA2P + + + +* Unpack scalar and vector parameters + PMT = AMPRMS(1) + GR2E = AMPRMS(8) + AB1 = AMPRMS(12) + DO I=1,3 + EB(I) = AMPRMS(I+1) + EHN(I) = AMPRMS(I+4) + ABV(I) = AMPRMS(I+8) + END DO + +* Spherical to x,y,z + CALL slDS2C(RM,DM,Q) + +* Space motion (radians per year) + PXR = PX*AS2R + W = VF*RV*PXR + EM(1) = -PR*Q(2)-PD*COS(RM)*SIN(DM)+W*Q(1) + EM(2) = PR*Q(1)-PD*SIN(RM)*SIN(DM)+W*Q(2) + EM(3) = PD*COS(DM) +W*Q(3) + +* Geocentric direction of star (normalized) + DO I=1,3 + P(I) = Q(I)+PMT*EM(I)-PXR*EB(I) + END DO + CALL slDVN(P,PN,W) + +* Light deflection (restrained within the Sun's disc) + PDE = slDVDV(PN,EHN) + PDEP1 = PDE+1D0 + W = GR2E/MAX(PDEP1,1D-5) + DO I=1,3 + P1(I) = PN(I)+W*(EHN(I)-PDE*PN(I)) + END DO + +* Aberration (normalization omitted) + P1DV = slDVDV(P1,ABV) + W = 1D0+P1DV/(AB1+1D0) + DO I=1,3 + P2(I) = AB1*P1(I)+W*ABV(I) + END DO + +* Precession and nutation + CALL slDMXV(AMPRMS(13),P2,P3) + +* Geocentric apparent RA,Dec + CALL slDC2S(P3,RA,DA) + RA = slDA2P(RA) + + END |