Description Usage Arguments Details Value Author(s) See Also Examples
Convert between celestial and Galactic (or Supergalactic) proper motion and coordinates
1 2 |
ra |
Right Ascension, in decimal hours (or decimal degrees if degree is set), scalar or vector |
dec |
declination, in decimal degrees, scalar or vector |
mu_ra |
Right Ascension proper motion, in any proper motion unit (angle/time), scalar or vector |
mu_dec |
declination proper motion, in any proper motion unit (angle/time), scalar or vector |
year |
equinox of ra and dec, scalar |
gl |
Galactic longitude, decimal degrees, scalar or vector |
gb |
Galactic latitude, decimal degrees, scalar or vector |
mu_gl |
Galactic longitude proper motion, in any proper motion unit (angle/time), scalar or vector |
mu_gb |
Galactic latitude proper motion, in any proper motion unit (angle/time), scalar or vector |
j |
integer indicator, direction of conversion |
degree |
if set, then the RA parameter (both input and output) is given in degrees rather than hours (default=FALSE) |
fk4 |
if set, then the celestial (RA, Dec) coordinates are assumed to be input/output in the FK4 system. By default, coordinates are assumed to be in the FK5 system. (default=FALSE) |
supergalactic |
if set, the function returns SuperGalactic coordinates (see details). (default=FALSE) |
mustar |
see details (default=FALSE) |
If j=1, this function converts proper motion in equatorial coordinates (ra,dec) to proper motion in Galactic coordinates (gl, gb) or Supergalactic Coordinates (sgl,sgb). If j=2, the conversion is reversed from Galactic/Supergalactic coordinates to equatorial coordinates. The calculation includes precession on the coordinates, but does not take care of precession of the proper motions which is usually a very small effect.
For B1950 coordinates, set fk4=TRUE and year=1950.
If supergalactic=TRUE is set, Supergalactic coordinates are defined by de Vaucouleurs et al. (1976) to account for the local supercluster. The North pole in Supergalactic coordinates has Galactic coordinates l = 47.47, b = 6.32, and the origin is at Galactic coordinates l = 137.37, b = 0.00.
If mustar=TRUE is set, the input and output of mu_ra and mu_dec are the projections of mu in the ra or dec direction rather than the d(ra)/dt or d(mu)/dt. So mu_ra becomes mu_ra*cos(dec) and mu_gl becomes mu_gl*cos(gb).
ra |
Right Ascension, in decimal hours (or decimal degrees if degree is set), scalar or vector |
dec |
declination, in decimal degrees, scalar or vector |
mu_ra |
Right Ascension proper motion, in any proper motion unit (angle/time), scalar or vector |
mu_dec |
declination proper motion, in any proper motion unit (angle/time), scalar or vector |
year |
equinox of ra and dec, scalar |
gl |
Galactic longitude, decimal degrees, scalar or vector |
gb |
Galactic latitude, decimal degrees, scalar or vector |
mu_gl |
Galactic longitude proper motion, in any proper motion unit (angle/time), scalar or vector |
mu_gb |
Galactic latitude proper motion, in any proper motion unit (angle/time), scalar or vector |
Written by Ed Shaya (Univ Maryland))2009.
R adaptation by Arnab Chakraborty June 2013
1 2 3 4 5 6 7 8 9 | # Find the SuperGalactic proper motion of M33 given its
# equatorial proper motion mu* =(-29.2, 45.2) microas/yr.
# Here the (*) indicates ra component is actual mu_ra*cos(dec)
# (Position: RA (J2000): 01 33 50.9, Dec (J2000): 30 39 35.8)
# Result: SGL = 328.46732 deg, SGB = -0.089896901 deg
# mu_sgl = 35.02 microarcsecond/yr, mu_sgb = 38.09 microarcsecond/yr.
glactc_pm(ten(1,33,50.9), ten(30,39,35.8), -29.2, 45.2, 2000,
gl, gb, mu_gl, mu_gb, 1)
|
$gl
[1] 133.6103
$gb
[1] -31.33086
$mu_gl
[1] -38.97888
$mu_gb
[1] 39.60733
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