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Table 3

Best fit model properties.

dusty ratran


Source p r0 n0 rout nout ν1000b b log10 (Gcr)
(AU) (108 cm-3) (103 AU) (104 cm-3) (km s-1) (km s-1) (Fisrf)

IRAS4A 1.8 33.5 30.5 11.2 8.7 1.1 ± 0.2 0.4 ± 0.1 –4.00 ± 0.25
L1527 0.9 5.4 0.9 6.5 15.0a 0.4 ± 0.2 0.9 ± 0.1 –4.25 ± 0.25
BHR71 1.7 24.8 9.4 12.4 2.4 1.3 ± 0.3 0.2 ± 0.1 –4.50 ± 0.25
IRAS 15398 1.4 6.1 19.4 4.9 17.1a 0.9 ± 0.2 0.7 ± 0.1 –4.25 ± 0.25
GSS30-IRS1 1.6 16.2 1.2 5.9 1.0 1.0 ± 0.3 0.8 ± 0.1 –3.50 ± 0.50
Ser-SMM4 1.0 12.1 7.9 12.5 43.1a 6.0 ± 0.6 0.7 ± 0.1 –4.00 ± 0.25
L1157 1.6 14.4 17.4 9.8 5.1 1.4 ± 0.5 0.3 ± 0.1 –4.75 ± 0.25

Notes.

(a)

Gisrf = 0 due to high outer density.

(b)

ν1000 is the infall velocity extrapolated to 1000 AU. In the case of Ser-SMM4 this seems too high to be reasonable. The implications of these results are discussed further in Sect. 4.3.

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