1999AJ....117..792S


Query : 1999AJ....117..792S

1999AJ....117..792S - Astron. J., 117, 792-810 (1999/February-0)

The structure and dynamics of the early-type resonance ring galaxy IC 4214. II. Models.

SALO H., RAUTIAINEN P., BUTA R., PURCELL G.B., COBB M.L., CROCKER D.A. and LAURIKAINEN E.

Abstract (from CDS):

The first paper in this series presented optical (UBVI) and near-infrared (H) surface photometry and Hα Fabry-Perot interferometry of IC 4214, an excellent example of a multiringed galaxy with a weak bar. In the present paper, we analyze the nonaxisymmetric gravitational potential of IC 4214, as defined by the near-infrared data. The gas behavior is modeled with two-dimensional sticky particle simulations that employ a rigidly rotating nonaxisymmetric potential. Our goals are to interpret the morphology and velocity field of IC 4214 and to obtain a model from which the bar pattern speed, halo contribution, and relative bulge and disk masses can be deduced. We also study the orbital families in the derived IC 4214 model.

A fairly good match, in both morphology and kinematics, is obtained for Ωbar~40±5 km.s–1.kpc–1, placing the bar corotation slightly beyond the end of the bar (rbar/rcr~0.72±0.05). The deduced bar amplitude implies that the visible mass of the disk dominates over the unseen halo (Mdisk/Mhalo>3-4). Moreover, our model accounts quantitatively for the large difference in the orientation of IC 4214 as derived in our first paper with photometric and kinematic methods.


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Journal keyword(s): Galaxies: Individual: Alphanumeric: IC 4214 - Galaxies: Kinematics and Dynamics - galaxies: photometry - galaxies: structure

Simbad objects: 3

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Number of rows : 3
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 NGC 4314 LIN 12 22 32.0223000912 +29 53 43.814812200 11.72 11.43 10.58     ~ 494 1
2 IC 4214 AG? 13 17 42.6918273984 -32 06 06.103910340   12.15 11.65 10.72 13.84 ~ 121 1
3 NGC 7217 LIN 22 07 52.3984675584 +31 21 33.632293572   12.94 11.92     ~ 511 0

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