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Table 6:

Linear radii, masses, and H2 column and volume-averaged number densities of the submm clumps within the IRDC G304.74.
  $R_{\rm eff}$ $M_{\rm cont}$ $N_{870}({\rm H_2})$ $N_{8}({\rm H_2})$   $\langle n({\rm H_2}) \rangle$
Source [pc] [ $M_{\hbox{$\odot$ }}$] [1022 cm-2] [1022 cm-2] N870/N8 [104 cm-3]
SMM 1a 0.42 107 $2.06\pm0.13$ $0.74\pm0.30$ $2.8\pm1.1$ 0.7
SMM 2b 0.33 53 $1.35\pm0.14$ $0.54\pm0.27$ $2.5\pm1.3$ 0.7
SMM 3c 0.49 182 $2.24\pm0.13$ 0.14d $16\pm0.9$ 0.7
SMM 4e 0.44 219 $2.96\pm0.13$ $0.36\pm0.24$ $8.2\pm5.5$ 1.2
IRAS 13037-6112 0.30 48 $1.17\pm0.07$ - - 0.8
SMM 5 0.30 37 $0.85\pm0.13$ $1.79\pm0.57$ $0.5\pm0.2$ 0.6
SMM 6 0.35 96 $2.06\pm0.13$ - - 1.0
SMM 7 0.35 48 $1.17\pm0.14$ $1.74\pm0.56$ $0.7\pm0.2$ 0.5
IRAS 13039-6108 0.47 78 $1.18\pm0.08$ - - 0.3
SMM 8 0.34 59 $1.39\pm0.13$ $2.23\pm0.76$ $0.6\pm0.2$ 0.7
SMM 9 0.37 85 $1.70\pm0.13$ $3.13\pm1.40$ $0.5\pm0.2$ 0.8
IRAS 13042-6105 0.31 43 $0.94\pm0.13$ - - 0.7

Notes. (a) By assuming $T_{\rm d}=30$ K (see Sect. 4.3 and Table 4), $M_{\rm cont}=39~M_{\odot}$, $N_{870}({\rm H_2})=0.75\pm0.05\times10^{22}$ cm-2, $N_{870}/N_{8}=1.0\pm0.1$, and $\langle n({\rm H_2}) \rangle=0.2\times10^4$ cm-3.
(b) By assuming $T_{\rm d}=30$K, $M_{\rm cont}=20~M_{\odot}$, $N_{870}({\rm H_2})=0.49\pm0.05\times10^{22}$cm-2, $N_{870}/N_{8}=0.9\pm0.1$, and $\langle n({\rm H_2}) \rangle=0.3\times10^4$ cm-3.
(c) By assuming $T_{\rm d}=30$K, $M_{\rm cont}=66~M_{\odot}$, $N_{870}({\rm H_2})=0.82\pm0.05\times10^{22}$cm-2, $N_{870}/N_{8}=5.9\pm0.4$, and $\langle n({\rm H_2}) \rangle=0.3\times10^4$ cm-3.
(d) No error given because it is greater than the actual value.
(e) By assuming $T_{\rm d}=30$K, $M_{\rm cont}=80~M_{\odot}$, $N_{870}({\rm H_2})=1.08\pm0.05\times10^{22}$cm-2, $N_{870}/N_{8}=3.0\pm2.0$, and $\langle n({\rm H_2}) \rangle=0.4\times10^4$ cm-3.


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