2004ApJ...606..483L


Query : 2004ApJ...606..483L

2004ApJ...606..483L - Astrophys. J., 606, 483-496 (2004/May-1)

Magnetohydrodynamic models of the bipolar knotty jet in Henize 2-90.

LEE C.-F. and SAHAI R.

Abstract (from CDS):

A remarkably linear, bipolar, knotty jet was recently discovered in Hen 2-90, an object classified as a young planetary nebula. Using two-dimensional, magnetohydrodynamic simulations, we investigate periodic variations in jet density and velocity as the mechanism for producing the jet and its knotty structures. From a detailed comparison between the Hα emission derived from our models and the observations, we find that a nonmagnetized jet with density or velocity variations does not reproduce in detail the observed structure of the Hen 2-90 jet–a magnetized jet with periodic velocity variations is required. This jet has a radius of 125 AU, an average velocity of 300 km/s with periodic variations (period = 43 yr) in the jet velocity of amplitude ±15 km/s, and a toroidal magnetic field with a characteristic strength of 0.6 mG. The average mass-loss rate in the jet has decreased by about a factor of 3 in 600 yr (i.e., from 4.7x10–7 M☉/yr at 20" to 1.7x10–7 M☉/yr at 1" from the center along the jet axis). The progenitor asymptotic giant branch wind is assumed to have a mass-loss rate of 1.5x10–6 M☉/yr (derived from the round, tenuous, Hα halo surrounding the central source) and a typical expansion velocity of 10 km/s. We find a fairly detailed similarity in the physical properties of the jet in Hen 2-90 with that in the young stellar object HH 34. This similarity suggests that the jets in both objects may be launched in a similar manner, namely, from an accretion disk, despite the fact that these objects are at very different evolutionary stages.

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Journal keyword(s): Stars: AGB and Post-AGB - Stars: Winds, Outflows

Simbad objects: 2

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Number of rows : 2
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HH 34 HH 05 35 31.30 -06 28 43.0     16     ~ 493 2
2 WRAY 16-125 PN 13 09 36.2390615830 -61 19 35.976251345   14.508 13.517 13.568   B[e] 128 0

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