Table 2:

SED fit parameters and results.
  T* L* $T_{\rm in}$ R* $R_{\rm out}/R_{\rm in}$ $R_{\rm in}$ $\dot{M}_{\rm total}$ $T_{\rm dust}^{\rm sub-mm}$ $M_{\rm dust}^{\rm sub-mm}$
  (104 K) ( $10^5~L_\odot$) (K) ($R_\odot$)   (km) ( $M_\odot~{\rm yr}^{-1}$) (K) ($M_\odot$)

R71 (inner/outer shell)
1.5 4.6 490/120 100 2/1.6 $\sim$1011/1012 $\sim$10-6 / $\sim$10-4 $9 \pm 1$ $\gtrsim$10-1
IRAS05280-6910 0.3 2.2 250 1700 30 $\sim$1011 $\sim$10-3 ... ...
HD 36402 18 4.6 960 15 300 $\sim$1010 $7\times10^{-6}$ ... ...
HD 36402 IR1 (YSO2) ... ... ... ... ... ... ... 64/15 ($\pm 1$) 10-12/> $1.5 \pm 0.4$

Notes. Fitting results from 2-D UST. DUSTY fits for R71 and IRAS05280-6910 estimate outer shell MLRs 2$\times$ to 4$\times$ less than the 2-D UST results. IR1/YSO2 was fit with two modified blackbodies (64 K and 15 K). For R71, we use O-deficient silicate optical constants (Ossenkopf et al. 1992) at long wavelengths and astronomical silicate optical constants (Draine & Lee 1984) at $\lambda <
0.18$ $\mu $m. For IRAS05280-6910, we use Ossenkopf et al. (1992) O-deficient silicates and for HD 36402, we use amorphous carbon grains from Zubko et al. (1996). The 2-D UST models use a KMH grain size distribution (Kim et al. 1994) with $a_{\rm min}=0.01~\mbox{$\mu$ m}$ and $a_0=0.1~\mbox{$\mu$ m}$ ( $a_0=1~\mbox{$\mu$ m}$ for IRAS05280-6910). Stellar parameters for R71 are consistent with those from Lennon et al. (1993). $T_{\rm dust}^{\rm sub-mm}$ is the temperature of the coldest dust component. For IRAS5280-6910, $\upsilon_{\rm
wind}$ is measured from the maser emission (20 km s-1; Marshall et al. 2004). For R71, we use 10 km s-1, but the velocity measured from the H$\alpha $ profile indicates the inner shell velocity may be >10$\times$ larger (Stahl et al. 1986). For HD36402, a typical velocity for a WC4 star is assumed (3000 km s-1; Willis et al. 2004).


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