Table 4: Derived physical quantities.
Jet lobe $r_0^{\rm a}$ $v_K^{\rm b}$ $\vert\dot{L}_{{\rm jet,min}}\vert^{\rm c}$ $\dot{L}_{{\rm disk,max}}^{\rm d}$ $\xi^{\rm e}$ $\lambda^{\rm e}$ $B_{\phi}/B_{\rm p}^{\rm f}$
  (AU) (km s-1) ($M_{\odot}$ yr-1 AU km s-1) ($M_{\odot}$ yr-1 AU km s-1)      
Red 1.58 $\pm$ 0.36 27.0 $\pm$ 3.2 $2.4 \pm 0.8 \times 10^{-5}$   0.025 $\leq \xi \leq $ 0.046 $12 \leq \lambda \leq $ 21 3.8 $\pm$ 1.1
        6.6 $\pm 1.5 \times 10^{-5}$      
Blue 0.44 $\pm$ 0.10 51.2 $\pm$ 6.2 $2.0 \pm 0.9 \times 10^{-5}$   0.037 $\leq \xi \leq $ 0.041 13 $\leq \lambda \leq $ 15 -8.9 $\pm$ 2.7
$^{{\rm a}}$
Derived with the method in Anderson et al. (2003).
$^{{\rm b}}$
Keplerian velocity at the footpoints r0.
$^{{\rm c}}$
Imposing that $\vert B_{\phi}\vert=0$ at the location of the observations and adopting the scalings in Ferreira & Pelletier (1993) (see text).
$^{{\rm d}}$
Considering only the portion of the disk from where the outflow seen at optical wavelengths originates.
$^{{\rm e}}$
Assuming dominant magnetic torque; accuracy 20-22%.
$^{{\rm f}}$
At about 80 AU above the disk and 30 (20) AU from the axis for the red (blue) lobe. Coordinate system as in Table 3.


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