2012A&A...538A.116S


Query : 2012A&A...538A.116S

2012A&A...538A.116S - Astronomy and Astrophysics, volume 538A116-116 (2012/2-1)

Comparison of synthetic maps from truncated jet-formation models with YSO jet observations. II. The effect of varying inclinations.

STUTE M. and GRACIA J.

Abstract (from CDS):

Analytical radially self-similar models are the best available solutions describing disk-winds, but they need several improvements. In a previous article, we introduced models of jets from truncated disks, i.e. evolved in time numerical simulations based on a radially self-similar MHD solution but including the effects of a finite radius of the jet-emitting disk, hence the outflow. In Paper I of this series, we compared these models with available observational data by varying the jet density and velocity, the mass of the protostar, and the radius of this truncation. In Paper I, we assumed that the jet lies in the plane of the sky. In this paper, we investigate the effect of different inclinations of the jet. To compare our models with observed jet widths inferred from recent optical images taken with HST and AO, we again created emission maps in different forbidden lines, and from such emission maps determined the jet width as the full-width half-maximum of the emission. We can reproduce the jet width of DG Tau and its variations very well, and the derived inclination of 40° is in excellent agreement with literature values of 32-52°. In CW Tau we overestimate the inclination in our best-fit model. In the other objects, we cannot find appropriate models that reproduce the variations in the observed jet widths. Only the average jet width itself is well modeled. We conclude that truncation - i.e. taking the finite radius of the jet launching region into account - is needed to reproduce the observed jet widths, and our simulations limit the possible range of truncation radii. The effects of inclination are important for modeling the intrinsic variations seen in observed jet widths. Our models can be used to infer the inclinations in the observed sample independently; however, a parameter study with a finer grid of parameters is needed.

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Journal keyword(s): methods: numerical - magnetohydrodynamics (MHD) - stars: pre-main sequence - ISM: jets and outflows

Simbad objects: 9

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Number of rows : 9
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 V* CW Tau TT* 04 14 17.0042670144 +28 10 57.766508508 13.92 13.64 12.36 12.86   K0Ve 381 0
2 V* DG Tau TT* 04 27 04.6921275888 +26 06 16.060169268 13.57 13.97 10.50 12.28   K6Ve 1092 1
3 V* V1213 Tau Or* 04 31 37.5055489536 +18 12 24.383952396           K7 605 0
4 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1546 0
5 IRAS 04287+1807 mul 04 31 38.8 +18 13 57           ~ 797 0
6 V* UZ Tau B TT* 04 32 42.8118779016 +25 52 31.198173600   14.07 12.72 13.35   M1/3Ve 158 0
7 V* HN Tau Or* 04 33 39.3629421552 +17 51 52.289234280   14.76 13.40 13.05   K5e 271 0
8 V* RW Aur TT* 05 07 49.5662483 +30 24 05.177426   10.86 9.60 9.95   K1/5e+K5e 816 0
9 HH 34 HH 05 35 31.30 -06 28 43.0     16     ~ 493 2

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