\begin{table}%tA.4
\caption{"Distance-independent'' parameters of the clumps. The angular diameters,
$\theta$, and integrated flux densities, $F_{\nu}$, have been derived from the 
1.2~mm continuum maps; the rotation temperatures, $T_{\rm rot}$, the \CIII~column 
densities, $N_{\rm C^{17}O}$, and the H$_{2}$~total column densities, 
$N_{\rm H_{2}}$, have been derived from {C$^{17}$O}~line ratios 
(assuming a~\CIII~mean abundance of 3.9~$\times$ $10^{-8}$); the ${\rm H}_{2}$~volume 
densities, $n_{\rm H_2}$, have been obtained from CS~line ratios.}
\label{tdist_ind}
%\centering
\par
\begin{tabular}{ccccccc}
\hline \hline
Source & $\theta$ & $F_{\nu}$ & $T_{\rm k}$ & $N_{\rm C^{17}O}$ & $N_{\rm H_2}$ & 
$n_{\rm H_2}$ \\
       &  (\asec ) & (Jy) & (K) & ($\times10^{15}$\cmq ) & (\cmq ) & (\cmc ) \\
\hline
08211$-$4158 & 34.3 & 2.26 & 12 & 2.3 & 5.9 $\times$ $10^{22}$ & 1.2 $\times$ $10^{5}$ \\
08563$-$4225 & 29.5 & 4.09 & 10 & 7.6 & 1.9 $\times$ $10^{23}$ & 1.7 $\times$ $10^{5}$ \\
09014$-$4736 & 42.1 & 0.79 &      &           &          &  \\
09026$-$4842 & 65.8 & 1.25 & 15 & 1.0 & 2.5 $\times$ $10^{22}$ & 6.3 $\times$ $10^{5}$ \\
09131$-$4723 & 71.6 & 4.5  & 14 & 1.7 & 4.3 $\times$ $10^{22}$ & 4.2 $\times$ $10^{5}$ \\
09166$-$4813 &    &  & 11 & 0.4 & 1.1$10\times^{22}$ &  \\
09209$-$5143 & 64.5 & 1.43 &     &          &           & \\
10095$-$5843 & 33.9 & 1.16 & 9 & 1.8 & 4.7 $\times$ $10^{22}$ & 1.5 $\times$ $10^{5}$ \\
10123$-$5727 & 43.2 & 2.41 &    &       &    & 1.7 $\times$ $10^{5}$ \\
10277$-$5730 & 27.0 & 0.63 &     &           &           & 4.9 $\times$ $10^{4}$ \\
10308$-$6122 & 33.8 & 0.45 &     &           &           & 2.1 $\times$ $10^{5}$ \\
10439$-$5941 & 42.8 & 6.90 &     &           &           & \\
10521$-$6031 & 6.5  & 0.46 &     &           &           & \\
10548$-$5929 & 65.5 & 0.62 &     &           &           & 5.2 $\times$ $10^{4}$ \\
10554$-$6237 & 21.5 & 0.73 & 8 & 2.9 & 7.4 $\times$ $10^{22}$ & 4.0 $\times$ $10^{4}$ \\
10572$-$6018 & 37.5 & 1.31 &     &           &           & 4.2 $\times$ $10^{4}$ \\
11265$-$6158 & 30.3 & 0.50 &     &           &           & 2.1 $\times$ $10^{5}$ \\
11294$-$6257 & 17.9 & 0.27 &     &           &           & \\
11380$-$6311 & 51.1 & 2.53 &     &           &           & 1.8 $\times$ $10^{5}$ \\
11404$-$6215 & 9.5  & 0.70 &     &           &           & \\
12295$-$6224 & 45.9 & 2.4  & 11 & 1.6 & 4.2 $\times$ $10^{22}$ & 1.4 $\times$ $10^{5}$ \\
12377$-$6237 & 15.1 & 0.53 &     &           &           & \\
13023$-$6213 & 28.5 & 1.39 &     &           &           & \\
13039$-$6108 & 50.9 & 1.38 & 18 & 0.7 & 1.9 $\times$ $10^{22}$ & 1.7 $\times$ $10^{5}$  \\
13106$-$6050 & 33.5 & 1.95 & 8 & 4.5 & 1.1 $\times$ $10^{23}$ & 5.7 $\times$ $10^{4}$  \\
13333$-$6234 & 31.8 & 1.5  & 8 & 3.7 & 9.4 $\times$ $10^{22}$ & 2.2 $\times$ $10^{5}$ \\
13384$-$6152 & 30.0 & 0.45 & 9 & 4.2 & 1.1 $\times$ $10^{23}$ & \\
13395$-$6153 & 24.5 & 4.2  & 10 & 6.8 & 1.7 $\times$ $10^{23}$ & 8.9 $\times$ $10^{4}$ \\
13438$-$6203 & 33.4 & 3.9  & 6 & 1.8 & 4.7 $\times$ $10^{22}$ & \\
13481$-$6124 & 25.5 & 7.12 & 18 & 2.8 & 7.1 $\times$ $10^{22}$ & 1.2 $\times$ $10^{5}$ \\
13560$-$6133 & 18.5 & 3.1  & 7 & 6.0 & 1.6 $\times$ $10^{23}$ & 1.5 $\times$ $10^{5}$ \\
14000$-$6104 & 50.5 & 4.4  & 11 & 1.3 & 3.3 $\times$ $10^{22}$ & 4.2 $\times$ $10^{5}$ \\
14131$-$6126 & $\ll$$21$ ($^{\#}$)  & 0.27  & 6 & 43.0 & 1.1 $\times$ $10^{24}$ & 1.7 $\times$ $10^{5}$ \\
14166$-$6118 & 48.9 & 1.06 & 8 & 2.4 & 6.1 $\times$ $10^{22}$ & 7.1 $\times$ $10^{4}$ \\
14183$-$6050 & 38.4 & 0.35 &     &           &           & 1.7 $\times$ $10^{5}$ \\
\hline
14201$-$6044 &   &  & 23 & 1.3 & 3.4 $\times$ $10^{22}$ &  \\
14395$-$5941 & $\ll 21$ ($^{\#}$)  & 0.46 & 6 & 46.1 & 1.2 $\times$ $10^{24}$ & 2.8 $\times$ $10^{4}$ \\
14425$-$6023 & 20.7 & 1.46 & 8 & 7.4 & 1.9 $\times$ $10^{23}$ & \\
15038$-$5828 &   &  & 17 & 0.6 & 1.6 $\times$ $10^{22}$ & \\
15072$-$5855 & 23.6 & 1.02 & 8 & 4.8 & 1.2 $\times$ $10^{23}$ & 1.2 $\times$ $10^{5}$ \\
15100$-$5903 & 28.  & 0.95 & 5 & 2.4 & 6.2 $\times$ $10^{22}$ & 2.8 $\times$ $10^{4}$ \\
15219$-$5658 & 15.2 & 0.52 &   &           &           & 5.3$10^{4}$ \\
15246$-$5612 & 20.2 & 1.26 & 7 & 8.4 & 2.2 $\times$ $10^{23}$ & 4.5 $\times$ $10^{4}$ \\
15262$-$5541 & 46.9 & 1.82 & 10 & 0.5 & 1.3 $\times$ $10^{22}$ & \\
15347$-$5518 & 48.4 & 3.12 & 8 & 2.1 & 5.3 $\times$ $10^{22}$ & 2.2 $\times$ $10^{5}$ \\
15371$-$5458 & 43.3 & 0.67 &     &           &          & 3.5 $\times$ $10^{5}$ \\
15470$-$5419 & 39.5 & 2.41 & 7 & 3.1 & 8.0 $\times$ $10^{22}$ & 2.0 $\times$ $10^{5}$ \\
15519$-$5430 & 32.1 & 6.38 & 12 & 6.4 & 1.6 $\times$ $10^{23}$ & 2.8 $\times$ $10^{5}$ \\
15557$-$5337 & 38.9 & 16.7 & 18 & 10.3 & 2.6 $\times$ $10^{23}$ & 3.7 $\times$ $10^{4}$ \\
15579$-$5303 & 21.3 & 6.26 & 6 & 9.2 & 2.4 $\times$ $10^{23}$ & \\
15583$-$5314 & 39.3 & 0.53 & 10 & 2.7 & 6.9 $\times$ $10^{22}$ & 1.3 $\times$ $10^{5}$ \\
16061$-$5048 & 27.7 & 1.64 & 6 & 4.8 & 1.2 $\times$ $10^{23}$ & \\
16082$-$5031 & 35.1 & 0.54 & 7 & 3.6 & 9.2 $\times$ $10^{22}$ & \\
16093$-$5015 & 34.8 & 1.81 & 8 & 2.9 & 7.5 $\times$ $10^{22}$ & 8.4 $\times$ $10^{4}$ \\
16093$-$5128 & 43.0 & 1.28 & 8 & 2.1 & 5.5 $\times$ $10^{22}$ & \\
16106$-$5048 &  &  & 11 & 0.8 & 2.0 $\times$ $10^{22}$ &  \\
16107$-$4956 &  &  & 6 &  0.4 & 1.1 $\times$ $10^{22}$ &  \\
16148$-$5011 & 12.4 & 2.32 & 8 & 11.6 & 3.0 $\times$ $10^{23}$ & \\
16187$-$4932 & 35.2 & 0.66 &     &           &           & \\
16194$-$4934 &  &  & 7 & 1.3 & 3.3 $\times$ $10^{22}$ &  \\
16204$-$4916 & 32.0 & 1.37 & 8 & 2.2 & 5.7 $\times$ $10^{22}$ & 2.4 $\times$ $10^{4}$ \\
16218$-$4931 & 16.4 & 0.69 & 6 & 10.1 & 2.6 $\times$ $10^{23}$ & 2.6 $\times$ $10^{4}$ \\
16232$-$4917 & 16.6 & 0.45 &     &           &           & 4.5 $\times$ $10^{4}$ \\
16252$-$4853 & 43.1 & 1.22 & 6 & 1.2 & 3.2 $\times$ $10^{22}$ & 2.4 $\times$ $10^{4}$ \\
16254$-$4844 &  &  & 12 & 1.1 & 2.9 $\times$ $10^{22}$ &  \\
16344$-$4605 & 26.6 & 2.85 & 7 & 4.7 & 1.2 $\times$ $10^{23}$ & \\
16363$-$4645 & 13.0 & 0.22 &     &     &        & 5.7 $\times$ $10^{4}$ \\
16369$-$4810 &  & & 8 & 1.8 & 4.7 $\times$ $10^{22}$ &  \\
16403$-$4614 &  & & 8 & 0.5 & 1.3 $\times$ $10^{22}$ & \\
16419$-$4602 & 17. & 2.27 & 9 & 2.1 & 5.3 $\times$ $10^{22}$ & \\
16464$-$4359 & 42. & 1.4  & 10 & 2.3 & 5.9 $\times$ $10^{22}$ & 7.1 $\times$ $10^{4}$ \\
16501$-$4314 & 70.9 & 2.15 & 15 & 1.7 & 4.3 $\times$ $10^{22}$ & 1.0 $\times$ $10^{5}$ \\
16535$-$4300 & 42.0 & 0.87 & 8 & 2.5 & 6.5 $\times$ $10^{22}$ & 3.5 $\times$ $10^{4}$ \\
17033$-$4035 &  &  & 15 & 1.5 & 3.7 $\times$ $10^{22}$ &  \\
\hline
17036$-$4033 &  &  & 10 & 0.7 & 1.9 $\times$ $10^{22}$ &  \\
17040$-$3959 & 15.6 & 0.95 & 7 & 8.5 & 2.2 $\times$ $10^{23}$ & 2.4 $\times$ $10^{4}$ \\
17082$-$4114 & 50. & 7.13 & 8 & 3.1 & 7.9 $\times$ $10^{22}$ & \\
17156$-$3607 &  &  & 10 & 0.8 & 2.0 $\times$ $10^{22}$ &  \\
17211$-$3537 & 36.8 & 1.1 & 7 & 1.6 & 4.2 $\times$ $10^{22}$ & 5.5 $\times$ $10^{4}$ \\
17218$-$3704 & 45.4 & 1.44 & 9 & 1.7 & 4.3 $\times$ $10^{22}$ & 1.7 $\times$ $10^{5}$ \\
17225$-$3426 &  &  & 10 & 1.7 & 4.3 $\times$ $10^{22}$ &  \\
17230$-$3531 & 21.6 & 1.19 & 7 & 10.9 & 2.8 $\times$ $10^{23}$ & 4.2 $\times$ $10^{4}$ \\
17256$-$3631 & 18.7 & 5.6 & 45 & 2.0 & 5.2 $\times$ $10^{22}$ & 7.1 $\times$ $10^{4}$ \\
17285$-$3346 & 11.9 & 0.26 &      &           &           & \\
17338$-$3044 & 19.0 & 0.19 &      &           &           & \\
17355$-$3241 & 45.5 & 0.6 & 8 & 2.2 & 5.7 $\times$ $10^{22}$ & 4.2 $\times$ $10^{4}$ \\
17377$-$3109 & 17.5 & 2.0 & 6 & 22.7 & 5.812 $\times$ $10^{23}$ & 1.1 $\times$ $10^{5}$\\
17410$-$3019 & 18.7 & 0.16 & 7 & 8.2 & 2.1 $\times$ $10^{23}$ & \\
17425$-$3017 & 21.1 & 1.59 & 7 & 5.1 & 1.3 $\times$ $10^{23}$ & 2.7 $\times$ $10^{4}$ \\
\hline
\end{tabular}
\medskip
$^{\#}$ Unresolved sources.
\end{table}