2001AJ....122.1508B


Query : 2001AJ....122.1508B

2001AJ....122.1508B - Astron. J., 122, 1508-1524 (2001/September-0)

Kinematics of optical outflows in the Orion nebula. I. The giant outflow HH 400 and the irradiated jet HH 502.

BALLY J., JOHNSTONE D., JONCAS G., REIPURTH B. and MALLEN-ORNELAS G.

Abstract (from CDS):

We present narrowband filter and high-resolution, velocity-resolved Fabry-Perot images of outflows in the southern portion of the Orion Nebula. HH 400 is a giant, low-velocity, redshifted bow shock located about 10' south of the core of the Orion Nebula. Its axis of symmetry passes close to the Trapezium cluster 1.5 pc to the north. The most likely point of origin is a young stellar object in the OMC-1 cloud core. HH 400 may be the remnant of a parsec-scale bipolar outflow powered by one of the young stars forming within this region. The radial velocity of gas in the limb-brightened rim of HH 400 is low, with redshifted speeds ranging from 8 to 20 km.s–1 with respect to the emission from the Orion Nebula. The shape of the bow indicates that it lies close to the plane of the sky. For an inclination angle of 30° to the plane of the sky and assuming that the plasma is flowing mostly along the axis of symmetry, the visible gas at the rim of HH 400 has a mean velocity of about 30 km.s–1, a mass of about 3x10–2 M, and a dynamical age of about 5x104 yr, assuming the source lies in the OMC-1 cloud core. The estimated mass flux in the HH 400 bow is about 10–6 M yr–1. The bent bipolar irradiated jet HH 502 is superposed on the western rim of HH 400. We resolve the spatial and velocity structure of the jet and its multiple bow shocks. The jet consists of a chain of photoionized segments separated by wide gaps; bow shocks lie at the leading edges of these jet segments. The mean radial velocities of the jet segments decrease with increasing distance from the source. The large radial velocity dispersions of the gas at the tips of the HH 502 internal working surfaces and the small spreading angles of the HH 502 jet segments, combined with their low radial velocities, indicate that this flow lies close to the plane of the sky. Assuming that the jet is fully ionized, that it spreads at the Mach angle, and that the internal sound speed in the photoionized gas is about 10 km.s–1, the jet must have a space velocity of about 400 km.s–1. Finally, we present velocity-resolved images of the bow shocks in HH 540, a flow that may originate from the large protoplanetary disk 181-826. Several additional high-velocity features identified in the Fabry-Perot data trace additional jets and outflows in this portion of the Orion Nebula.

Abstract Copyright:

Journal keyword(s): ISM: Herbig-Haro Objects - ISM: individual (Orion Nebula) - ISM: Jets and Outflows - Stars: Formation - Stars: Pre-Main-Sequence

Nomenclature: Table 3: [BJJ2001b] HH 559 Knot N (Nos 1-3), [BJJ2001b] LL Ori 6 A (Nos A-B).

Simbad objects: 45

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Number of rows : 45
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* LL Ori Or* 05 35 05.6361678504 -05 25 19.520320800 12.997 12.309 11.517   10.034 K0-K3e 108 1
2 HH 269 HH 05 35 09.1 -05 23 44           ~ 42 0
3 HH 202 HH 05 35 11.5 -05 22 46           ~ 72 4
4 HH 201 HH 05 35 11.5 -05 21 54           ~ 38 2
5 HH 205 HH 05 35 11.703 -05 20 24.69           ~ 33 0
6 NAME OMC-1 MoC 05 35 14 -05 22.4           ~ 1169 2
7 HH 558 HH 05 35 14.5 -05 31 07           ~ 1 0
8 [LB2000] 154-041 * 05 35 15.45928 -05 20 40.6911           ~ 52 0
9 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1619 1
10 M 42 HII 05 35 17 -05 23.4           ~ 4074 0
11 NAME Ney-Allen Nebula ISM 05 35 17.1 -05 23 18           ~ 28 0
12 HH 540 HH 05 35.3 -05 31           ~ 9 0
13 V* V2323 Ori Or* 05 35 18.1042843896 -05 28 25.086577692   18.990 18.772 16.09 16.157 M1:e 37 1
14 NAME Beehive Proplyd Y*? 05 35 18.50 -05 28 24.4           ~ 22 1
15 HH 540B HH 05 35 19.2 -05 29 58           ~ 2 0
16 HH 540A HH 05 35 19.5 -05 31 06           ~ 2 0
17 HH 561 HH 05 35 20.3 -05 30 40           ~ 3 0
18 HH 540C HH 05 35 20.7 -05 31 30           ~ 2 0
19 HH 203 HH 05 35 22.2 -05 24 58           ~ 71 4
20 HH 204 HH 05 35 22.6 -05 25 13           ~ 79 4
21 COUP 1238 * 05 35 23.1000221088 -05 28 37.189602804 18.288 19.541 19.659   17.899 ~ 10 0
22 HH 560 HH 05 35.4 -05 29           ~ 2 0
23 HH 559 HH 05 35.4 -05 28           ~ 1 0
24 HH 400W1 HH 05 35 24.8 -05 29 07           ~ 1 0
25 HH 400W2 HH 05 35 25.0 -05 30 00           ~ 1 0
26 HH 560N HH 05 35 25.4 -05 28 41           ~ 1 1
27 HH 502S7 HH 05 35 26.0 -05 30 54           ~ 5 0
28 HH 502S6 HH 05 35 26.1 -05 30 39           ~ 4 0
29 HH 560M HH 05 35 26.4 -05 29 17           ~ 1 1
30 HH 502S5 HH 05 35 26.6 -05 30 17           ~ 4 0
31 HH 502S4 HH 05 35 27.0 -05 30 04           ~ 4 0
32 HH 502S1 HH 05 35 27.5 -05 29 45           ~ 4 0
33 HH 502 HH 05 35 27.9 -05 29 35           ~ 10 0
34 HH 560S HH 05 35 28.6 -05 30 13           ~ 3 1
35 HH 502N2 HH 05 35 30.1 -05 28 55           ~ 5 0
36 HH 400W4 HH 05 35 30.4 -05 30 46           ~ 1 0
37 HH 400W3 HH 05 35 30.6 -05 30 49           ~ 1 0
38 HH 502N3 HH 05 35 30.8 -05 28 43           ~ 5 0
39 HH 400 HH 05 35 34 -05 30.5           ~ 9 0
40 HH 400E2 HH 05 35 34.2 -05 29 23           ~ 1 0
41 HH 400W5 HH 05 35 34.3 -05 31 52           ~ 1 0
42 HH 400W6 HH 05 35 34.4 -05 31 55           ~ 1 0
43 HH 400E3 HH 05 35 34.4 -05 29 25           ~ 1 0
44 HH 400E1 HH 05 35 34.4 -05 29 25           ~ 1 0
45 HH 400W7 HH 05 35 34.6 -05 31 55           ~ 1 0

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