F. Shu et al., MAGNETOCENTRIFUGALLY DRIVEN FLOWS FROM YOUNG STARS AND DISKS .1. A GENERALIZED-MODEL, The Astrophysical journal, 429(2), 1994, pp. 781-796
We propose a generalized model for stellar spin-down, disk accretion,
and truncation, and the origin of winds, jets, and bipolar outflows fr
om young stellar objects. We consider the steady state dynamics of acc
retion of matter from a viscous and imperfectly conducting disk onto a
young star with a strong magnetic field. For an aligned stellar magne
tosphere, shielding currents in the surface layers of the disk prevent
stellar field lines from penetrating the disk everywhere except for a
range of radii about omegaBAR = R(x), where the Keplerian angular spe
ed of rotation OMEGA(x) equals the angular speed of the star OMEGA. F
or the low disk accretion rates and high magnetic fields associated wi
th typical T Tauri stars, R(x) exceeds the radius of the star R by a
factor of a few, and the inner disk is effectively truncated at a radi
us R(t) somewhat smaller than R(x). Where the closed field lines betwe
en R(t) and R(x) bow sufficiently inward, the accreting gas attaches i
tself to the field and is funneled dynamically down the effective pote
ntial (gravitational plus centrifugal) onto the star. Contrary to comm
on belief, the accompanying magnetic torques associated with this accr
eting gas may transfer angular momentum mostly to the disk rather than
to the star. Thus, the star can spin slowly as long as R(x) remains s
ignificantly greater than R. Exterior to R(x) field lines threading t
he disk bow outward, which makes the gas off the midplane rotate at su
per-Keplerian velocities. This combination drives a magnetocentrifugal
wind with a mass-loss rate M(w) equal to a definite fraction f of the
disk accretion rate M(D). For high disk accretion rates, R(x) is forc
ed down to the stellar surface, the star is spun to breakup, and the w
ind is generated in a manner identical to that proposed by Shu, Lizano
, Ruden, & Najita in a previous communication to this journal. In two
companion papers (II and III), we develop a detailed but idealized the
ory of the magnetocentrifugal acceleration process.