We present an analysis of disk-resolved images of Io at 232.5, 260, an
d 285 mn taken with the FOC (Faint Object Camera) of the Hubble Space
Telescope. The images at 232.5 and 260 mn were acquired in 1993 in an
effort to separate the surface and SO2 atmosphere contributions to the
observed UV albedo. We combine these images to make UV color maps of
the regions centered on the leading and trailing hemispheres. Between
latitudes +60 degrees and -60 degrees we find that the UV colors are d
ominated by three distinctive components, B-0, B-1, and B-2, one more
than was found to be required to fit visible wavelength Voyager data a
t these latitudes. The Voyager component ''B'' (McEwen, A. S., T. V. J
ohnson, D. L. Matson, and L. A. Sonderblom 1988. Icarus 75, 450-478) a
ppears to be a combination of two distinct spectral components: B-1 an
d B-2. We find that B-1, the darker component, represents either a new
compositional unit or patches of SO2 vapor overlying compositional un
it B (= B-2). To distinguish between these two possibilities, we propo
se two simple models of surface reflectivities and SO2 vapor curve of
growth designed to allow a crude separation between the effects of the
absorptions by surface materials and SO2 vapor. In Model 1, we recogn
ize that all absorption bandmodels share a linear regime at the limit
of small absorption path-lengths and assume that the SO2 vapor absorpt
ion spectrum on Io is linearly dependent on absorption pathlength at a
ll wavelengths without temperature dependencies. In this case Io's alb
edo must be dominated by the surface reflectance and the spectral diff
erences between B-1 and B-2 are the signature of different surface uni
ts. In this model the two-way SO2 vapor column density is either below
our detectability limit of similar to 4.10(17) mol . cm(-2) or is con
fined to denser patches below our spatial resolution limit of similar
to 250 km. In Model 2, we recognize that SO2 absorptions on Io may be
non-linear at 285 nm (a local maximum in SO2 absorption cross sections
) even in the presence of significant transmission through the gas. We
retain the assumption of linearity at 232.5 mn where the SO2 absorpti
on cross sections are smallest and consider two variants of the model
in which different assumptions are made about the underlying albedo of
the surface materials. In variant A, which is characterized by a rela
tively high assumed UV reflectivity for SO2 frost, the amounts of gas
are inconsistent with mm-wave and UV spectroscopic observations, and w
ith the cold temperatures found for the pervasive thermal reservoir un
it in Veeder et al.'s (Veeder, G. J., D. L. Matson, T. V. Johnson, D.
L. Blaney, and J. D. Goguen 1994. J. Geophys. Res. (Planets) 99, 17095
-17162) thermophysical model of the surface. In variant B, SO2 frost i
s characterized by the lowest UV reflectivity consistent with the data
. In this case there is no detectable SO2 vapor over SO2 frost rich re
gions and the FOC UV images are consistent with the presence of SO2 va
por in patches of column density N similar to 10(18) cm(-2) covering s
imilar to 11-15% of Io's projected surface. This variant of Model 2 is
found to be in agreement with both the disk integrated UV spectroscop
ic and mm-wave observations and Veeder et al.'s thermophysical model.
In particular the longitude distribution of the SO2 patches is similar
to the longitude distribution of thermal anomalies in Veeder et al.'s
model. The identification of the composition of the B unit remains pr
oblematic. Polysulfur oxides (PSO) give a reasonable accounting of the
UV reflectivities but may be too bright near 700 nm; Sulfur does not
satisfy the UV albedos but cannot be ruled out because of uncertaintie
s in its behavior under Io conditions. In any of the above models, reg
ardless of the assumptions made concerning the curve of growth of SO2
vapor absorption, we find that the percentage coverage of SO2 frost in
the regions of Io's surface that we observed is in the range of 50-60
%. This is a similar result to those found in earlier spectroscopic st
udies of SO2 frost features near 2 and 4 mu m. (C) 1996 Academic Press
, Inc.