![]() | Annu. Rev. Astron. Astrophys. 1978. 16:
103-39 Copyright © 1978 by Annual Reviews. All rights reserved |
3.2. Rotation Curves in the Outer Parts of Spiral Galaxies
Radio measurements of the HI 21-cm line velocities in galaxies have
considerably increased the radial distance to which rotation curves
can be obtained; optically derived rotation curves rarely extend
beyond ~ 1/3RHo, while in HI they often reach beyond
RHo. Before such
observations were available it was usually assumed that at large radii
the rotation curves eventually became Keplerian,
Vrot
R-1/2. In fact
actual rotation curves are now found to decline much more slowly or
even not at all
(Roberts 1975b,
Huchtmeier 1975,
Combes et al. 1977).
Bosma (1978a,
b)
has recently analyzed HI velocity fields in a sample
of about 20 galaxies, based on data from new observations with the
WSRT and on results available in the literature. His results can be
summarized as follows: The rotation curves are almost always either
flat or slowly declining in the outer parts.
(3)
Construction of mass
models shows indeed that out to the last observed point the total mass
Mout still does not converge to an asymptote.
The ratio
Mout/Ltot is about 5-15 independent
of type (H0 = 75
km/sec/Mpc) indication in a number of galaxies that
Mout/Ltot has a
tendency to increase with radius. However, Bosma cautions that, given
the uncertainties arising from noncircular motions, beam smoothing,
thin disk approximation, etc, these results should be considered as
very tentative.
Krumm & Salpeter (1977; see also Salpeter 1978) have extended the HI rotation curves of six mainly edge-on spiral galaxies to even larger distances (84 kpc for NGC 4565 if H = 50 km/sec/Mpc) using the Arecibo radio telescope. They find further evidence that Vrot refuses to decrease in the outer parts of these galaxies; however, the very existence of HI there disagrees in two notable cases with observations made with the WSRT (NGC 4565 and 4631, Sancisi 1978) so that these results require further verification.
Rotation curves that remain high at large distances imply increasing M/L ratios in the outer parts of galaxies. Indeed, if the surface brightness continues the exponential decrease found in the brighter parts of the disk (e.g. Freeman 1970a) and the rotation curve remains constant with R, then Mout/Ltot is proportional to R. Roberts & Whitehurst (1975) derived local M/L values of 200 or more at 30 kpc radius in M31, assuming that the HI velocities that they measured were due to pure rotation and taking a particular model for the mass distribution [see also Roberts (1976)]. Observations of M31 at Cambridge (Emerson & Baldwin 1973) seemed at first to indicate that the rotation curve differed from that derived by Roberts and Whitehurst; however, a more recent analysis (Emerson 1976, Newton & Emerson 1977) has removed the discrepancy. Furthermore, Newton and Emerson conclude that the high degree of (anti-) symmetry of the velocity field on either side of the minor axis of M31 strongly suggests that the observed velocities indeed result from rotation, to better than 10 km/sec.
Finally, we discuss briefly the question of whether the forms of the
rotation curves provide any evidence for massive halos around
galaxies. It is certainly true that more mass is waiting to be found
beyond the last measured HI points on many rotation curves; the values
of a few × 1011
M
currently quoted for Luminosity Class I and II
galaxies refer to radii of 20-50 kpc. However, the great increase
(factors of 10 to 100) in masses advocated by
Einasto et al. (1974)
and by Ostriker et
al. (1974)
involve estimates at much greater radial
distances, from 200-500 kpc. As has been stated by
Turner & Ostriker
(1977),
there is no evidence in favour of such massive halos within
the visible disks of galaxies; the standard rotation curve analyses
give values of Mout at some R that differ by
only ~ 20% if one assumes
a spherical rather than a flattened mass distribution. Nevertheless,
it is a fact that not a single galaxy has been found with a Keplerian
rotation curve at large R. We must conclude that the results from
rotation curves are not inconsistent with the existence of extensive,
massive halos around galaxies, although the prime evidence for them
comes from studies of binary galaxies and outlying globular clusters (e.g.
Turner & Ostriker
1977,
Sargent 1977).
3 A notable exception to this general statement is M81 (Rots 1975), where the observed rotation curve on the northwest side begins to increase again beyond about 10 kpc. A convenient excuse for this may be found in a postulated interaction of M81 with M82 and NGC 3077 (see Section 4.6 below). The observed rotation curve on the southeast side continues to decline. Back.