There have been a wide variety of LMC censuses, most of which treat
the LMC as a galaxy and use the standard mass and mass density
estimates: rotation curves, star counts, surface brightness profiles.
Two relatively recent rotation curve studies, Meatheringham et al.
(1988) and Schommer et al.
(1992), estimate LMC masses of
and
.
Similar limits follow
from carbon star studies by Kunkel et al.
(1997b). The main difference between these
determinations is not the value of Vc for the Cloud but the radial
extent of the rotation curve. Alternatively, from the Milky Way's
point of view, the LMC is similar to an oversized globular cluster.
Its tidal radius is measurable and depends on both the Milky Way
rotation curve and the LMC mass (and, weakly, its profile). A
preliminary estimate of the tidally inferred LMC mass (Nikolaev &
Weinberg 1998) yields
but is consistent with the Schommer et al.
estimate. A brief description of this result is provided in the
Appendix.
Recent estimates of the LMC space velocity from archival plate (Jones
et al. 1994) and Hipparcos (Kroupa &
Bastian 1997) proper motions both lead to
consistent estimates of the LMC orbital plane. The procedure used
here to estimate the orbit is described in Weinberg
(1995). For the Milky Way halo, I choose a
W0=3 King model (1966) with
and mass
scaled to
(Kochanek 1996).
The rotation curve due to the Galaxy, then, is approximately flat in
the region of the LMC orbit. Together with a disk, the overall
rotation curve is a plausible representation of the observed Milky
Way. With this halo model, both the space velocities estimated by
Jones et al. and Kroupa & Bastian yield a similar perigalacticon of
46 kpc with apogalacticons of 72 kpc and 120 kpc. For lack of
motivation to favor one of these over the other, I adopt the mean
apogalacticon.