A SUPERSHELL MODEL FOR THE HIGH-VELOCITY AND INTERMEDIATE-VELOCITY NEUTRAL HYDROGEN CLOUDS

Authors
Citation
Gl. Verschuur, A SUPERSHELL MODEL FOR THE HIGH-VELOCITY AND INTERMEDIATE-VELOCITY NEUTRAL HYDROGEN CLOUDS, The Astrophysical journal, 409(1), 1993, pp. 205-233
Citations number
55
Categorie Soggetti
Astronomy & Astrophysics
Journal title
ISSN journal
0004637X
Volume
409
Issue
1
Year of publication
1993
Part
1
Pages
205 - 233
Database
ISI
SICI code
0004-637X(1993)409:1<205:ASMFTH>2.0.ZU;2-8
Abstract
The velocities and spatial distribution of high- and intermediate-velo city neutral hydrogen gas in the second quadrant of Galactic longitude in the northern hemisphere are accounted for in terms of a model in w hich the ''clouds'' appear to be part of a vast supershell with an ell iptical cross section normal to the Galactic disk. Its origin appears to be in the Perseus arm toward l = 131-degrees +/- 4-degrees with an apparent radius of 1920 pc and an expansion velocity of 281 +/- 10 km s - 1. The supershell is treated, to first order, as an elongated stru cture coaxial with the Perseus spiral arm in order to facilitate compa rison between available high-velocity cloud (HVC) velocities and the m odel. Further observations of intermediate-velocity H I are essential for refining the characteristics of the supershell model in three dime nsions. If the supershell is uniformly filled with gas, the total mass of H I is 3.2 x 10(6) M. with kinetic energy 2.5 x 10(54) ergs. This is greater than values found in other supershells. If, instead, the ga s is filamentary with typical structures less-than-or-equal-to 5 pc wi de, the total energy is less-than-or-equal-to 2.0 x 10(53) ergs. Gas i n the near side of the shell could be as close as 30 pc from the Sun. However, in the solar neighborhood the supershell has impacted a local structure marked by the radio continuum spur known as Loop III. Evide nce is presented that the incoming stream of high-velocity gas from th e Perseus arm has been decelerated at the surface of Loop III, which t herefore acts to modulate the observed distribution of HVCs. Taking in to account the influence of Loop III, the parameters describing the su pershell are derived by comparing model predictions with the latitude- velocity distribution of the HVCs in 5-degrees longitude intervals usi ng data from the Hulsbosch & Wakker survey. The model is then used to predict the spatial distribution of the H I brightness in several velo city regimes and compared with the Bell Laboratories H I survey data. The good agreement between the model and the northern hemisphere data suggests that the brightest HVCs result from column density enhancemen ts occurring over a large depth in space, in many cases of order sever al hundred parsecs. An exception appears to be stream A, which may rep resent gas still being decelerated at the interface between the supers hell and loop III. The distances to the high- and intermediate-velocit y H I structures follow from the model. Distances are dependent on loc ation and velocity, ranging from 100 pc or less for gas in the near fa ce of the supershell in directions away from Loop III to as much as 1 kpc for material in the - 100 km s-1 regime in certain directions. Fin ally, it is suggested that high-latitude, low-velocity H I and molecul ar ''clouds'' and their associated cirrus structures result from trans ient density enhancements at the interface between the incoming stream of high-velocity material associated with the supershell and loop III .