Table 2: Conversion factors of the line intensity in erg s-1 cm-2 into the velocity integrated main beam temperature $T_{\rm mb} \Delta v$ observed at the IRAM and JCMT telescopes respectively, for the five lines observed towards IRAS 16293-2422 (Parise et al. 2005). Last column quotes the $T_{\rm mb} \Delta v$ observed towards IRAS 16293-2422 (Parise et al. 2005).a Predicted flux from the model simply converted into K km s-1 using the conversion factor. b Predicted flux derived using an accurate convolution of the signal with the telescope beam.

Transition
Frequency Telescope Conversion coeff IRAS 16293-2422
  (GHz)   1 K km s-1 ( $T_{\rm mb} \Delta v$) (K km s-1) (K km s-1) (K km s-1)
      (erg s-1 cm-2) Conversiona Convolutionb Obsc

11,0-11,1
80.578 IRAM 1.4 $\times $ 10-17 0.19 0.21 0.40
31,2-22,1 225.897 IRAM 4.1 $\times $ 10-17 1.7 1.8 1.7
21,1-21,2 241.561 IRAM 4.4 $\times $ 10-17 1.5 1.5 2.0
22,0-31,3 266.161 IRAM 4.9 $\times $ 10-17 0.20 0.22 0.21
10,1-00,0 464.924 JCMT 4.0 $\times $ 10-16 6.3 5.4 5.5


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