Документ взят из кэша поисковой машины. Адрес
оригинального документа
: http://www.naic.edu/~phil/mbeam/Tsys/cmpTsysFromArchive.html
Дата изменения: Thu Aug 18 00:08:32 2005 Дата индексирования: Sat Dec 22 17:04:49 2007 Кодировка: |
The system temperature is computed from
the calon (tsys + Tcal) and the caloff (Tsys) scans. The
processing is normally:
caloff
TsysK= ------------ * calK
(calOn - calOff)
This is the same as:
let calRatio=calOn/caloff
1.
(1.)
TsysK= ---------- * calK
calratio - 1
Rfi in the cal on or cal off can cause problems in the
computation.
It is best to ignore frequency bins that contain rfi. Fitting the
band pass and removing outliers is hard because of the iflo bandpass
shape. The ratio calon/caloff does not have this problem.
Using the following definitions:
Tsky - sky temp, Gsky frquency dependence of sky
temp
Tcal - cal temp, Gcal frequency dependence
of the cal
Tiflo - power from the omt,amps. iflo, Giflo frequency
dependence
The the cal ratio can be written as:
(Tsky*Gsky + Tcal*Gcal + Tiflo )*Giflo
calRatio= ---------------------------
(Tsky*Gsky + Tiflo )*Giflo
So Giflo cancels. If you assume that Tsky,Gsky is the same for
the on/off
then you get:
(Tcal*Gcal)
calRatio - 1 = --------------
(Tsky*Gsky + Tiflo )
Since Gcal,Gsky is a slowly varying function of frequency (we're
ignoring standing waves since they have little power in them) you can
do a low order fit and throw out any outliers (nsig above the fit residuals).
The procedure is then: