Abstract
The most accurate measurements of magnetic fields in star-forming gas are
based on the Zeeman observations analyzed by Crutcher et al. (2010). We show
that their finding that the 3D magnetic field scales approximately as
density\$^0.65\$ can also be obtained from analysis of the observed
line-of-sight fields. We present two large-scale AMR MHD simulations of several
thousand \$M\_ødot\$ of turbulent, isothermal, self-gravitating gas, one with a
strong initial magnetic field (Alfven Mach number \$M\_A,0= 1\$) and one with a
weak initial field (\$M\_A,0=10\$). We construct samples of the 100 most massive
clumps in each simulation and show that they exhibit a power-law relation
between field strength and density in excellent agreement with the observed
one. Our results imply that the average field in molecular clumps in the
interstellar medium is \$<B\_tot> 42 n\_H,4^0.65 \mu\$G. Furthermore,
the median value of the ratio of the line-of-sight field to density\$^0.65\$ in
the simulations is within a factor of about (1.3, 1.7) of the observed value
for the strong and weak field cases, respectively. The median value of the
mass-to-flux ratio, normalized to the critical value, is 70\% of the
line-of-sight value. This is larger than the 50\% usually cited for spherical
clouds because the actual mass-to-flux ratio depends on the volume-weighted
field, whereas the observed one depends on the mass-weighted field. Our results
indicate that the typical molecular clump in the ISM is significantly
supercritical (\~ factor of 3). The results of our strong-field model are in
very good quantitative agreement with the observations of Li et al. (2009),
which show a strong correlation in field orientation between small and large
scales. Because there is a negligible correlation in the weak-field model, we
conclude that molecular clouds form from strongly magnetized (although
magnetically supercritical) gas.
Users
Please
log in to take part in the discussion (add own reviews or comments).