If your maps show simple source morphology and you are only interested
in integrated flux densities, the simplest approach is to calibrate
your map Jy/aperture for the aperture size you want to use. The
listing of FLUXES also gives us the total flux, S
for Uranus
at 850
m is 67.9 Jy. Let us first see how we can use this value
to calibrate our image in terms of Jy/arcsecond
. In order to do
this we need to derive a value for the Flux Conversion Factor (FCF)
which is in units of Jy/arcsecond
/V. To do this we first need to
work out the sum of the pixel values (V
) in an aperture of
radius r. We then find the FCF is given by
| (5) |
| Radius (arcseconds) | 20 | 30 | 40 | 60 | 120 |
| V |
45.75 | 60.76 | 64.89 | 70.07 | 77.08 |
| FCF (Jy/arcsecond |
1.48 | 1.12 | 1.05 | 0.97 | 0.88 |
We can see from this table that the FCF is dependent on the aperture size that is used 1 This is because there is significant signal in the sidelobes and extended error beam of the telescope. Clearly then the value of FCF can be somewhat ambiguous. What you have to remember is that if you are doing photometry of an extended object, you should use a value for the FCF derived for the same aperture.
If you need to use small apertures, i.e. the size of your HPBW, you will need
to use a point source or point like source as a calibrator. Flux densities
for our secondary calibrators for a 40'' aperture are given by Jenness et al.
[14]. However, several of our secondary calibrators are not point
sources. If you end up with, for example, IRC
10216 and IRAS 16293
2422
or Mars near perhelion as your only calibrators during your run, you are in
trouble. You may be able to use a large aperture to recover all the flux and
use the ratios between different apertures derived for a point source. But,
you may as well bite the bullet and calibrate in Jy/beam.
The SCUBA map reduction cookbook