ArticlePDF Available

Io Volcanism Seen by New Horizons: A Major Eruption of the Tvashtar Volcano

Authors:

Abstract and Figures

Jupiter's moon Io is known to host active volcanoes. In February and March 2007, the New Horizons spacecraft obtained a global snapshot of Io's volcanism. A 350-kilometer-high volcanic plume was seen to emanate from the Tvashtar volcano (62 degrees N, 122 degrees W), and its motion was observed. The plume's morphology and dynamics support nonballistic models of large Io plumes and also suggest that most visible plume particles condensed within the plume rather than being ejected from the source. In images taken in Jupiter eclipse, nonthermal visible-wavelength emission was seen from individual volcanoes near Io's sub-Jupiter and anti-Jupiter points. Near-infrared emission from the brightest volcanoes indicates minimum magma temperatures in the 1150- to 1335-kelvin range, consistent with basaltic composition.
Content may be subject to copyright.
NH Long Range Reconnaissance Imager (LORRI)
images (17). This same feature appears in the HST/
SBC image in Fig. 2B, obtained when East Girru
was shifted just behind the limb. The auroral feature
near East Girru in both LORRI and HST/SBC im-
ages is ~15° northward of Jupiters field line tangent
point at the limb, which suggests that ionospheric
currents are diverted northward from this nominal
position toward a region of higher gas density near
the plume. Similar deviations of the anti-jo vian FUV
emissions from nominal tangent points observed
with STIS are likely caused by the prevalence and
distribution of plumes there (21). Volcanic plume
aurorae were not identified in previous lower-quality
STIS FUV images, which caused an apparent dis-
crepancy with visible images of plume aurorae. The
East Girru plume FUV auroral feature in Fig. 2 re-
solves this discrepancy and reveals the influence of
plumes on Ios electrodynamic interaction. The
upstream-side emission feature is more apparent
when limb brightened at viewing geometries like
those reported in Fig. 2. This feature was predicted
by aurora image s imulations (22) and is diagnostic of
the diverg ence of the plasma flow upstream of Io, a
primary trait of Ios interaction with th e plas ma torus.
References and Notes
1. F. Bagenal, J. Atmos. Sol. Terres. Phys. 69, 387 (2007).
2. E.Lellouch,M.A.McGrath,K.L.Jessup,inIo After Galileo
(Springer-Praxis, UK, 2006), pp. 231264.
3. J. Pearl et al., Nature 280, 755 (1979).
4. W. M. Sinton, C. Kaminski, Icarus 75, 207 (1988).
5. J. R. Spencer et al., Science 288, 1198 (2000).
6. A. F. Cook et al., Science 211, 1419 (1981).
7. J. T. Clarke, J. Ajello, J. Luhmann, N. M. Schneider,
I. Kanik, J. Geophys. Res. 99, 8387 (1994).
8. P. E. Geissler et al., Science 285, 870 (1999).
9. A. H. Bouchez, M. E. Brown, N. M. Schneider, Icarus 148,
316 (2000).
10. P. E. Geissler et al., J. Geophys. Res. 106, 26137 (2001).
11. P. E. Geissler et al., Icarus 172, 127 (2004).
12. I. DePater et al., Icarus 156, 296 (2002).
13. K. D. Retherford, thesis, The Johns Hopkins University (2002).
14. J. Saur, D. F. Strobel, Icarus 171, 411 (2004).
15. S. A. Stern et al., in Astrobiology and Planetary Missions,
R. B. Hoover, G. V. Levin, A. Y. Rozanov, G. R. Gladstone,
Eds. (Proc. SPIE, Volume 5906, 2005), pp. 358367.
16. K. D. Retherford et al., paper presented at the
Magnetospheres of the Outer Planets Meeting, San
Antonio, TX, 25 June, 2007.
17. J. R. Spencer et al., Science 318, 240 (2007).
18. The angular size of Io varies with spacecraft distance but
is smaller than the Alice slit width for these data. The
spectral resolution varies between 0.3 nm and ~0.9 nm
for emissions known to be located near the satellite disk
(22); see, e.g., Fig. 2.
19. H. C. Ford et al., in Future EUV/UV and Visible Space
Astrophysics Missions and Instrumentation, J. C. Blades,
O. H. W. Siegmund, Eds. (Proc. SPIE, Volume 4854,
2003), pp. 8194.
20. F. L. Roesler et al., Science 283, 353 (1999).
21. K. D. Retherford et al., J. Geophys. Res. 105, 27157 (2000).
22. J. Saur, F. M. Neubauer, D. F. Strobel, M. E. Summers,
Geophys. Res. Lett. 27, 2893 (2000).
23. K. D. Retherford, H. W. Moos, D. F. Strobel, J. Geophys.
Res. 108, 1333 (2003).
24. L. M. Feaga, thesis, The Johns Hopkins University (2005).
25. K. L. Jessup et al., Icarus 169, 197 (2004).
26. J. R. Spencer et al., Icarus 176, 283 (2005).
27. P. D. Feldman et al., Geophys. Res. Lett. 27, 1787 (2000).
28. D. F. Strobel, B. C. Wolven, Astrophys. Space Sci. 277,
271 (2001).
29. F. Neubauer, J. Geophys. Res. 103, 19843 (1998).
30. F. M. Neubauer, J. Geophys. Res. 104, 3863 (1999).
31. We thank the New Horizons mission and science teams.
New Horizons is funded by NASA. Support for this work was
also provided by NASA though grant number GO-10871
from the Space Telescope Science Institute (STScI), which is
operated by the Association of Universities for Research in
Astronomy, Inc., under NASA contract NAS5-26555.
Supporting Online Material
www.sciencemag.org/cgi/content/full/318/5848/237/DC1
Figs. S1 and S2
Tables S1 and S2
10 July 2007; accepted 19 September 2007
10.1126/science.1147594
REPORT
Io Volcanism Seen by New Horizons:
A Major Eruption of the
Tvashtar Volcano
J. R. Spencer,
1
* S. A. Stern,
2
A. F. Cheng,
2
H. A. Weaver,
3
D. C. Reuter,
4
K. Retherford,
5
A. Lunsford,
4
J. M. Moore,
6
O. Abramov,
1
R. M. C. Lopes,
7
J. E. Perry,
8
L. Kamp,
7
M. Showalter,
9
K. L. Jessup,
1
F. Marchis,
9
P. M. Schenk,
10
C. Dumas
11
Jupiters moon Io is known to host active volcanoes. In February and March 2007, the New Horizons
spacecraft obtained a global snapshot of Ios volcanism. A 350-kilometer-high volcanic plume was seen to
emanate from the Tvashtar volcano (62°N, 122°W), and its motion was observed. The plumes
morphology and dynamics support nonballistic models of large Io plumes and also suggest that most
visible plume particles condensed within the plume rather than being ejected from the source. In images
taken in Jupiter eclipse, nonthermal visible-wavelength emission was seen from individual volcanoes near
Ios sub-Jupiter and anti-Jupiter points. Near-infrared emission from the brightest volcanoes indicates
minimum magma temperatures in the 1150- to 1335-kelvin range, consistent with basaltic composition.
T
he New Horizons (NH) Jupiter flyby pro-
vided the first close-up observations of the
tidally driven volcanism of Jupiters moon Io
since the last Galileo orbiter observations of Io in late
2001 (1). The closest approach to Io occurred at
21:57 UT on 28 February 2007 at a range of 2.24
million km. Sunlit observations were made at solar
phase angles from to 159°, and four eclipses of Io
by Jupiter were also observed. NH obtained 190 Io
images with its 4.96 mrad per pixel panchromatic
(400 to 900 nm) Long-Range Reconnaissance Im-
ager (LORRI) and 17 color nighttime and eclipse
images with the 20 mrad per pixel Multicolor V isible
Imaging Camera (MVIC), although MVIC coverage
of Ios day side was not possible because of detector
saturation. NH also obtained seven 1.25- to 2.5-mm
near-infrared image cubes at 62 mrad per pixel with
the Linear Etalon Infrared Spectral Array instrument
(LEISA) and numerous disk-integrated ultraviolet
observations with the Alice instrument, discussed
separately (2).
Eleven volcanic plumes were identified in the
NH images (Fig. 1A and table S1). In addition to the
single very large Pele-type plume at Tvashtar,
which is described separately , NH observed 10 SO
2
-
rich Prometheus-type plumes (35). These smaller
plumes averaged 80 km high and varied greatly in
brightness. Plumes seen for the first time by NH
include those at Zal and Kurdalagon and a large new
plume, 150 km high, at north Lerna Regio, which
has produced a large albedo change. Three of these
plumes, north Lerna and north and south Masubi,
are associated with recent large lava flows, sup-
porting the idea that Prometheus-type plumes
result from mobilization of surface volatiles by
active lava flows. All active plumes that were on
Table 2. Alice-measured emission line brightness averages and SDs in sunlight and eclipse.
Emission line Type
Disk-average brightness (rayleighs)
IEclipse01 IEclipse04 IEclipse05
OI 130.4 nm Sunlight 706 ± 134 445 ± 27 347 ± 142
Eclipse 597 ± 43 394 ± 14 254 ± 71
Ratio S/E 1.18 ± 0.24 1.12 ± 0.08 1.37 ± 0.68
OI 135.6 nm Sunlight 882 ± 177 577 ± 35 480 ± 188
Eclipse 797 ± 57 536 ± 18 381 ± 94
Ratio S/E 1.11 ± 0.24 1.08 ± 0.08 1.26 ± 0.58
SI 147.9 nm Sunlight 1167 ± 271 986 ± 54 596 ± 288
Eclipse 1205 ± 87 874 ± 28 429 ± 144
Ratio S/E 0.97 ± 0.24 1.13 ± 0.07 1.39 ± 0.82
12 OCTOBER 2007 VOL 318 SCIENCE www.sciencemag.org240
New Horizons at Jupiter
on January 26, 2009 www.sciencemag.orgDownloaded from
the disk or near the limb were also visible in
Jupiter eclipse images because of excitation of
plume gases by the jovian magnetosphere (Fig.
2B), as also seen by Galileo (6).
LORRI imaged almost all of Io at relatively low
phase angles with resolutions between 14 and 22 km
per pixel, providing a surface albedo map suitable for
comparison with previous maps (7) (Fig. 1A). There
are at least 19 locations where surface changes have
occurred since Galileos last global images, taken
between 1999 and 2001 (Fig. 1A). The number of
surface changes detected is only one-fourth of those
detected during the 5-year Galileo mission (8), per-
haps because of NHs lower spatial resolution, the
lack of a color data set with comparable resolution,
and the possibility of surface changes that have faded
since their formation.
The large plume at Tvashtar has renewed the
large ring-shaped plume deposit seen at Tvashtar in
2000 (1), which had been obscured by other plume
deposits by mid-2001. A two-lobed plume deposit
surrounds a new , 240-km-long dark feature, prob-
ably a lava flow, at Masubi (Fig. 1, B to D) created
by the two plumes observed by NH: North Masubi
near the vent and South Masubi at the distal flow
front. This flow is the longest new lava flow to be
erupted on Io since the 1979 Voyager images. The
North Lerna volcanic plume has produced a 700-km-
wide concentric deposit (Fig. 1, E and F) surround-
ing a fresh, 130-km-long apparent dark lava flow .
Other late-Galileo-era plume deposits, notably around
Dazhbog and Thor (8), have faded to invisibility.
LEISA observed 1.25- to 2.5-mm volcanic ther-
mal emission from Ios night side or in Jupiter eclipse
at almost all longitudes at a spatial resolution of 140
to 170 km per pixel, producing a uniform global
snapshot of Ios high-temperature volcanic thermal
emission (Fig. 1A). Thermal emission from several
volcanoes was also seen in 0.4- to 1.0-mmLORRI
images in Jupiter eclipse or on the night side (Fig.
2A). At least 36 hot spots were detected. All cor-
respond to pre viously known active volc anic centers
1
Southwest Research Institute, 1050 Walnut Street, Suite 300,
Boulder, CO 80302, USA.
2
NASA Headquarters, Washington, DC
20546, USA.
3
Applied Physics Laboratory, Johns Hopkins Uni-
versity, 11100 Johns Hopkins Road, Laurel, MD 20723, USA.
4
NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA.
5
Southwest Research Institute, Post Office Drawer 28510, San
Antonio, TX 78228, USA.
6
NASA Ames Research Center, Moffett
Field, CA 94035, USA.
7
Jet Propulsion Laboratory, 4800 Oak Grove
Drive, Pasadena, CA 91109, USA.
8
Lunar and Planetary Laboratory,
University of Arizona, Tucson, AZ 85721, USA.
9
Search for Extra-
terrestrial Intelligence (SETI) Institute, 515 North Whisman Road,
Mountain View, CA 94043, USA.
10
Lunar and Planetary Institute,
3600 Bay Area Boulevard, Houston, TX 77058, USA.
11
European
Southern Observatory, Casilla 19001, Santiago 19, Chile.
*To whom correspondence should be addressed. E-mail:
spencer@boulder.swri.edu
360 330 300 270 240 210 180 150 120 90 60 30 0
W. Longitude
−90
−60
−30
0
30
60
90
Latitude
A
Masubi
N. Lerna
Tvashtar
Zal
Amirani
Thor
Prometheus
Zamama
Marduk
Kurdalagon
B
α = 49
Masubi, Galileo
C
Masubi, NH
α = 31
D
Masubi, NH
α = 83
E
N. Lerna, Voyager
F
N. Lerna, NH
Fig. 1. (A) Global map of Io derived from eight LORRI images obtained at
phase angles between 26° and 47°, showing volcanic activity detected by NH.
See fig. S1 for an unannotated version. Yellow ovals denote areas with new,
faded, or shifted plume or other volatile deposits since the last Galileo images
in 2001. Green circles denote areas where probable new lava flows have
occurred. Cyan diamonds indicate locations of active plumes (table S1), and
orange hexagons are volcanic hot spots detected by LEISA. For plumes and hot
spots, symbol size indicates the approximate relative size and brightness of the
features. (B to F) Comparison of NH LORRI and earlier images (7)ofmajor
surface changes at Masubi (45°S, 57°W) and North Lerna (55°S, 290°W),
reprojected to a consistent geometry. The scale bars are 200 km long, and a is
the solar phase angle. At Masubi, old lava flows seen by Voyager and Galileo
(B) have been obscured at low phase angles (C) by plume deposits associated
with what is probably a new dark lava flow. The old flows are still seen by NH
at high phase angles (D), suggesting the plume deposits are not thick enough
to obscure the surface texture of the old flows. At North Lerna, a recent
eruption has generated a 130-km-long dark feature (F), probably a lava flow,
as well as an active plume that has produced a concentric pattern of deposits.
www.sciencemag.org SCIENCE VOL 318 12 OCTOBER 2007
241
SPECIALSECTION
on January 26, 2009 www.sciencemag.orgDownloaded from
(9) except for a bright new hot spot that we call East
Girru at 22°N, 235°W , 130 km east of the known
volcano Girru. This hot spot location corresponds to
an inconspicuous dark linear feature, possibly an old
fissure eruption, in Galileo images. No associated
albedo change is visible in sunlit LORRI images;
perhaps East Girru is a very young eruption that has
not had time to produce observable albedo cha nges.
No plume was seen in reflected light at East Girru,
but a detached glow 330 km directly abov e the hot
spot was seen in eclipse images (Fig. 2A), suggesting
some associated gas output.
LORRI eclipse images show numerous faint point
sources of emission (Fig. 2A), particularly near the
sub-jovian and anti-jovian points (on the equator at
longitudes and 180°W), with a typical brightness of
~100 kRayleigh assuming a 15-km-by-15-km source
region. These were also seen in Galileo eclipse images
(6). These spots all correspond to low-albedo volcanic
centers (Fig. 2D), but because simultaneous LEISA
images show no corresponding cluster of bright spots
in the near-infrared (Fig. 2, E and F), where volcanic
thermal emission dominates, it is likely that a non-
thermal mechanism, probably plasma-related, creates
the sub-jovian and anti-jovian clusters of point-source
emission. Most of these spots are less than about 30
km in size, suggesting a near-surface origin.
A fortuitous major eruption of the Tvashtar vol-
cano during the NH flyby provides a comprehen-
sive view of a large, sulfur- rich Pele-class (3)
volcanic plume on Io. Tvashtar, a series of calderas
centered near 62°N, 122°W, has been one of Ios
most active volcanos in recent years. An active
period from late 1999 to early 2001 (1012 )
produced a large infrared hot spot, plume, and
orange pyroclastic deposits and was followed by
quiescent conditions seen in late 2001 (1, 13)and
early 2003 and 2004. Renewed thermal emission in
April to May 2006 (14) may have been an earlier
phase of the 2007 eruption seen by NH. Continued
thermal emission from Tvashtar was seen by
ground-based observations during and after the NH
encounter from 18 January (15) to 27 May 2007.
The 2007 Tvashtar plume was first seen in back-
scattered light in 260-nm wavelength images from
the Hubble Space T elescope (HST) on 14 February
2007 (Fig. 3A) and again in absorption in Jupiter
transitimageson21February(Fig.3B).Absorption
in the 260-nm wavelength region suggests, by
analogy with previous HST observations of the Pele
plume, that the Tvashtar plume is rich in S
2
gas (16),
as also inferred from the orange color of its plume
deposits seen previously by Galileo (12, 17).
NH imaged the Tvashtar plume on 39 occasions
over 7.8 days, at phase angles between and 159°
and LORRI resolutions between 12 and 38 km per
pixel. The plume height was remarkably constant,
varying between roughly 320 and 360 km, and full
width was about 1100 km, consistent with the diam-
eter of the pyroclastic deposits (Fig. 1). The plume
had a bright top in all images (Fig. 3, C, D, and F to
J), very similar to Voyager images of the Pele plume:
This morphology is not consistent with simple bal-
listic models of plume particle flight, as noted for Pele
(18), but is consistent with hydrodynamic models
with entrained particles that include a gas shock front
at the top of the plume (19). Most Tvashtar plume
images show little evidence for a central upgoing
column of particles (e.g., Fig. 3C), suggesting that the
observed particles may condense out of the plume
rather than being directly ejected from the vent.
The plume contains remarkable time-variable
filamentary structures similar to those glimpsed in
the single high-resolution Voyager 1 image of the
Pele plume. This structure allows tracing of motion
within the plume in a sequence of five images of the
upper part of the plume obtained at 2-min intervals
on 1 March (Fig. 3, F to J, and movie S1). Speeds
projected on the plane of the sky are 0.4 to 0.7 km s
1
(Fig. 3E), comparable to expected ballistic ejection
speeds for a 350-km-high plume (~1.0 km s
1
), and
accelerate as plume features fall toward the surface.
Features appear to slide down the upper surface of
the plume rather than tracing ballistic trajectories
originating at the vent.
The source of the Tvashtar plume is associated
with by far the brightest hot spot seen by NH (Fig. 4).
A B
0
30
240
270
300
330
P
EG
C D
E
0
30
240
270
300
330
F
Fig. 2. Images of Io in Jupiter eclipse. (A) LORRI image taken at 27 February 14:37 UT with an effective
exposure time of 16 s. Dark blotches and straight lines are artifacts. The brightest spots (P, Pele; EG, East Girru)
are thermal emission from active volcanoes, and more diffuse emission is from the plumes and atmosphere (6).
(B) Same image with latitude/longitude grid showing glowing plumes (plume sources, table S1, indicated by
red diamonds). (C) Simulated sunlit view with the same geometry, based on sunlit LORRI images (Fig. 1A). (D)
Combined sunlit (cyan) and eclipse (red) image, showing that all pointlike sources of emission in the eclipse
image correspond to low-albedo volcanic centers. (E)A~2.3-mm LEISA eclipse image at 27 February 15:31 UT,
showing thermal emission from active volcanoes. Elongation of the hot spots is an artifact. (F) Combined visible
albedo (cyan) and LEISA thermal emission (red) image, showing the sources of the volcanic emission.
12 OCTOBER 2007 VOL 318 SCIENCE www.sciencemag.org
242
New Horizons at Jupiter
on January 26, 2009 www.sciencemag.orgDownloaded from
Thermal emission was observed on multiple occa-
sions by LORRI, LEISA, and by MVIC at wave-
lengths from 2.5 to below 0.7 mm. The hot spot
location, 62.5°N, 122.5°W , coincides with the fire
fountains seen at Tvashtar by Galileo in November
1999. The spectrum can be fit with a single tem-
perature blackbody at 1287 K from 1.25 to 2.04 mm,
providing a lower limit to the magma temperature,
comparable to Galileo estimates (12). Assuming a
temperature of 1200 K for the Tvashtar hotspot, an
area of 49 km
2
is derived from the brightness in
LORRI images, comparable to the ~25 km
2
area of
the incandescent fire fountain seen by Galileo at
Tvashtar in November 1999 (12). The isothermal
blackbody emission spectrum at close to magmatic
temperatures is also consistent with an energetic erup-
tion such as a fire fountain, rather than, for instance,
spreading and cooling lava flows (20, 21). T emper-
atures are consistent with basaltic lava composi-
tion: Exotic high temperature magmas, inferred from
some Galileo observations (22), are not required
either at Tvashtar or other hot spots seen by NH.
References and Notes
1. E. P. Turtle et al., Icarus 169, 3 (2004).
2. K. D. Retherford et al., Science 318, 237 (2007).
3. A. S. McEwen, L. Soderblom, Icarus 55, 191 (1983).
4. P. Geissler, D. Goldstein, in Io After Galileo,R.M.C.Lopes,
J. R. Spencer, Eds. (Praxis, Chichester, UK, 2007), pp. 163192.
5. Pele-type plumes are thought to result from direct
ejection of gas from a volcanic vent, whereas the
smaller Prometheus-type plumes may result from
remobilization of surface volatiles by lava flows.
6. P. E. Geissler et al., J. Geophys. Res. 106, 26137 (2001).
7. U.S. Geological Survey Astrogeology Research Program,
http://astrogeology.usgs.gov/Projects/JupiterSatellites/io.html.
8. P. E. Geissler et al., Icarus 172, 127 (2004).
9. R. M. C. Lopes, J. Radebaugh, M. Meiner, J. Perry,
F. Marchis, in Io After Galileo,R.M.C.Lopes,J.R.Spencer,
Eds. (Praxis, Chichester, UK, 2007), pp. 307323.
10. R. R. Howell et al., J. Geophys. Res. 106, 33129 (2001).
11. F. Marchis et al., Icarus 160, 124 (2002).
12. M. P. Milazzo et al., Icarus 179, 235 (2005).
13. F. Marchis et al., Icarus 176, 96 (2005).
14. C. Laver, I. de Pater, F. Marchis, Bull. Am. Astron. Soc.
38, 612 (2006).
15. J. A. Rathbun , J. R. Spencer, paper presented at the 39th
annual American Astronomical Society, Division for
Planetary Science meeting, Orlando, FL, 9 October 2007.
16. J. R. Spencer, K. L. Jessup, M. A. McGrath, G. E. Ballester,
R. Yelle, Science 288, 1208 (2000 ).
17. A. S. McEwen et al ., Icarus 135, 181 (1998).
18. R. G. Strom, N. M. Schneider, in Satellites of Jupiter,
D. Morrison, Ed. (Univ. of Ariz ona Press, Tucson, AZ,
1982), pp. 598633.
19. J. Zhang et al., Icarus 172, 479 (2004).
20. J. A. Stansberry, J. R. Spencer, R. R. Howell, D. Vakil,
Geophys. Res. Lett. 24, 2455 (1997).
21. A. G. Davies et al., J. Geophys. Res. 106, 33079 (2001).
22. A. S. McEwen et al ., Science 281, 87 (1998).
23. We thank the entire NH mission team, particularly D. Rose
and E. Birath, and our colleagues on the NH science team.
NH and the ancillary investigations described here are funded
by NASA, whose financial support we gratefully acknowledge.
Supporting Online Material
www.sciencemag.org/cgi/content/full/318/5848/240/DC1
Fig. S1
Table S1
Movie S1
10 July 2007; accepted 19 September 2007
10.1126/science.1147621
Fig. 3. The Tvashtar plume.
(A) Discovery image by HST
in backscattered light in the
F255W filter (central wave-
length = 260 nm). The red
diamond indicates the plume
source. (B) HST image of
260 nm absorption by the plume
against Jupiter: 260 nm (blue)
plus 330 nm (green) plus
410 nm (red) color compos-
ite. Other images are in visi-
ble light from NH LORRI. The
scale bar is 200 km long, and
the yellow star indicates the
projected location of the hot
spot at the plume source. The
dashed line is the terminator.
(C) Highest-resolution view of
the full plume, at a resolution
of 12.4 km per pixel and
phase angle of 102°, show-
ing the filamentary structure.
Images are sharpened by
unsharp masking: the dark
line at the edge of the disk is
an artifact of the sharpening.
(D) Image at 145° phase
angle at 22.4 km per pixel,
showing the time variability
of the details of the plume
structureandthepersistent
bright top. (F to J)Sequence
of frames at 2-min intervals
showing dynamics in the up-
perpartoftheplume(the
source is on the far side of
Io). Colored diamonds track
individual features whose
speeds, projected on the plane of the sky, are shown in (E).
F 03/01 23:50:31
G 03/01 23:52:31
H 03/01 23:54:31
I 03/01 23:56:31
J 03/01 23:58:31
C 02/28 11:04:22
D 03/02 06:07:22
E Plume speeds
0 2 4 6 8
Time, Minutes
0.
3
0.
4
0.
5
0.
6
0.
7
0.
8
Projected Speed, km/sec
A HST, 02/14 B HST, 02/21
Fig. 4. LEISA spectra of volcanic thermal emission from Tvashtar, Pele, and East Girru, with best-fit
blackbody curves superposed. Vertical axis units are GW steradian
1
mm
1
.
www.sciencemag.org SCIENCE VOL 318 12 OCTOBER 2007
243
SPECIALSECTION
on January 26, 2009 www.sciencemag.orgDownloaded from
... We compare our results with estimations and observations of the solar wind and Io activity during the observation intervals, in order to examine the effects of internal versus external factors on the location shifts of Ganymede's footprint. Evidence of persistently strong volcanic eruptions on Io from February to the beginning of June 2007 were presented by Spencer et al. (2007), Yoneda et al. (2009, and Yoneda et al. (2013). Spencer et al. (2007) revealed the continuous thermal emission from the Tvashtar plume from 18 January to 27 May 2007. ...
... Evidence of persistently strong volcanic eruptions on Io from February to the beginning of June 2007 were presented by Spencer et al. (2007), Yoneda et al. (2009, and Yoneda et al. (2013). Spencer et al. (2007) revealed the continuous thermal emission from the Tvashtar plume from 18 January to 27 May 2007. In addition, Bonfond et al. (2012) using auroral images of Jupiter's northern hemisphere from HST showed the expansion of the main emission on 31 May 2007 (equivalent to Day Of Year 151 or DOY 151) including the location of Ganymede's footprint which shifted ∼500 km in equatorward direction. ...
... For Case 1, Ganymede's footprint detected on DOY 054 shifted in the poleward direction in comparison to Ganymede's footprint detected on DOY 068. There were continuous volcanic eruptions on Io during February and March 2007 (Spencer et al., 2007). Therefore, the mass loading rate (̇) increased due to the additional volcanic materials from Io, resulting in an increase in cold plasma density in the magnetosphere, which affects the magnetic field line stretching and Ganymede's footprint locations detected on both DOY 054 and DOY 068. ...
Article
Full-text available
Variations of Ganymede's auroral footprint locations are presented based on observations by the Hubble Space Telescope in 2007 and 2016. The poleward and equatorward shifts of Ganymede's footprint could be influenced by the mass outflow rate from Io and the solar wind compression, as the internal and external factors respectively. We compare our results with Ganymede's footprint mapping based on the magnetodisc model. The mapped footprint in Jupiter's ionosphere shifts equatorward with increased hot plasma parameter, Kh, which is associated with hot plasma pressure. We analyzed the effect of cold plasma number density (Nc), related to the mass outflow rate and connected to the material produced by Io. The results show that the magnetic footprint is shifted equatorward by 0.37° when the mass outflow rate is increased from 800–2,000 kg s⁻¹. Iogenic plasma has a strong influence on the stretching of the magnetic field lines in Jupiter's middle magnetosphere, causing the equatorward shift of Ganymede's footprint. For external factors, Ganymede's footprint shifted poleward by 0.62° under the influence of solar wind compression while the mass outflow is kept constant at 1,000 kg s⁻¹. We present similar locations of Ganymede's footprint based on the field lines mapped as a result of the compensation between an increase of Kh and the solar wind compression. Overall, the location of Ganymede's auroral footprint corresponds with the mass loading rate from Io and the solar wind dynamic pressure.
... A sputtering component may contribute to the composition of it, see, e.g., [1,2]. In addition to outgassing and other supplies such as, for example, accretion, species may also originate active volcanism, e.g., [3,4], or plumes [5,6]. Impacting micrometeorites and radiation interaction with the surface lift surface material, micrometeorites and fractures thereof into the upper atmosphere forming dust clouds contain solid samples [7][8][9]. ...
... Regarding the complexity of molecules to be analyzed, two major groups of questions can be identified: on the one hand, fundamental questions on the origin and evolution of many Solar System objects can be revealed by analyzing atomic gas and simple molecules present in the exosphere [10]. Many of those species are known or at least expected to be present in various exospheres to at least some extent including CH 4 , CO, NH 3 , N 2 ; the noble gasses up to Xe and the isotopic ratios D/H, 3 He/ 4 He, 13 C/ 12 C, 15 N/ 14 N, 20 Ne/ 22 Ne, 38 Ar/ 36 Ar, ...
Article
Full-text available
Spacecraft flybys provide access to the chemical composition of the gaseous envelope of the planetary object. Typical relative encounter velocities range from km/s to tens of km/s in flybys. For speeds exceeding about 5 km/s, modern mass spectrometers analyzing the rapidly encountering gas suffer from intrinsic hypervelocity impact-induced fragmentation processes causing ambiguous results when analyzing complex molecules. In this case, instruments use an antechamber, inside which the incoming species collide many times with the chamber wall. These collisions cause the desired deceleration and thermalization of the gas molecules. However, these collisions also dissociate molecular bonds, thus fragmenting the molecules, and possibly forming new ones precluding scientists from inferring the actual chemical composition of the sampled gas. We developed a novel time-of-flight mass spectrometer that handles relative encounter velocities of up to 20 km/s omitting an antechamber and its related fragmentation. It analyzes the complete mass range of m/z 1 to 1000 at an instance. This innovation leads to unambiguous analysis of complex (organic) molecules. Applied to Enceladus, Europa or Io, it will provide reliable chemical composition datasets for exploration of the Solar System to determine its status, origin and evolution.
... Such limb topography was derived for Io (Thomas et al., 1998), saturnian icy satellites (Nimmo et al., 2010;Thomas, 2010), and Mercury (Oberst et al., 2011), to mention a few. Limb images were also used to estimate the height of ice and dust clouds on Mars (Hernández-Bernal et al., 2019;Sánchez-Lavega et al., 2015 and even the height of volcanic plumes on Io (Geissler and McMillan, 2008;Spencer et al., 2007;Strom et al., 1979). Closer to home, near-limb images from geostationary satellites were used to reconstruct the atmospheric trajectory of the 2013 Chelyabinsk meteor (Miller et al., 2013) and study the altitude of polar mesospheric clouds (Gadsden, 2000a(Gadsden, , b, 2001Proud, 2015;Tsuda et al., 2018). ...
Article
Full-text available
A geometric technique is introduced to estimate the height of volcanic eruption columns using the generally discarded near-limb portion of geostationary imagery. Such oblique observations facilitate a height-by-angle estimation method by offering close-to-orthogonal side views of eruption columns protruding from the Earth ellipsoid. Coverage is restricted to daytime point estimates in the immediate vicinity of the vent, which nevertheless can provide complementary constraints on source conditions for the modeling of near-field plume evolution. The technique is best suited to strong eruption columns with minimal tilting in the radial direction. For weak eruptions with severely bent plumes or eruptions with expanded umbrella clouds the radial tilt/expansion has to be corrected for either visually or using ancillary wind profiles. Validation on a large set of mountain peaks indicates a typical height uncertainty of ±500 m for near-vertical eruption columns, which compares favorably with the accuracy of the common temperature method.
Preprint
Full-text available
Decline and recovery timescales surrounding eclipse are indicative of the controlling physical processes in Io's atmosphere. Recent studies have established that the majority of Io's molecular atmosphere, SO2 and SO, condenses during its passage through Jupiter's shadow. The eclipse response of Io's atomic atmosphere is less certain, having been characterized solely by ultraviolet aurorae. Here we explore the response of optical aurorae for the first time. We find oxygen to be indifferent to the changing illumination, with [O I] brightness merely tracking the plasma density at Io's position in the torus. In shadow, line ratios confirm sparse SO2 coverage relative to O, since their collisions would otherwise quench the emission. Io's sodium aurora mostly disappears in eclipse and e-folding timescales, for decline and recovery differ sharply: ~10 minutes at ingress and nearly 2 hr at egress. Only ion chemistry can produce such a disparity; Io's molecular ionosphere is weaker at egress due to rapid recombination. Interruption of a NaCl+ photochemical pathway best explains Na behavior surrounding eclipse, implying that the role of electron impact ionization is minor relative to photons. Auroral emission is also evident from potassium, confirming K as the major source of far red emissions seen with spacecraft imaging at Jupiter. In all cases, direct electron impact on atomic gas is sufficient to explain the brightness without invoking significant dissociative excitation of molecules. Surprisingly, the nonresponse of O and rapid depletion of Na is opposite the temporal behavior of their SO2 and NaCl parent molecules during Io's eclipse phase.
Article
Full-text available
Decline and recovery timescales surrounding eclipse are indicative of the controlling physical processes in Io’s atmosphere. Recent studies have established that the majority of Io’s molecular atmosphere, SO 2 and SO, condenses during its passage through Jupiter’s shadow. The eclipse response of Io’s atomic atmosphere is less certain, having been characterized solely by ultraviolet aurorae. Here we explore the response of optical aurorae for the first time. We find oxygen to be indifferent to the changing illumination, with [O i ] brightness merely tracking the plasma density at Io’s position in the torus. In shadow, line ratios confirm sparse SO 2 coverage relative to O, since their collisions would otherwise quench the emission. Io’s sodium aurora mostly disappears in eclipse and e-folding timescales, for decline and recovery differ sharply: ∼10 minutes at ingress and nearly 2 hr at egress. Only ion chemistry can produce such a disparity; Io’s molecular ionosphere is weaker at egress due to rapid recombination. Interruption of a NaCl ⁺ photochemical pathway best explains Na behavior surrounding eclipse, implying that the role of electron impact ionization is minor relative to photons. Auroral emission is also evident from potassium, confirming K as the major source of far red emissions seen with spacecraft imaging at Jupiter. In all cases, direct electron impact on atomic gas is sufficient to explain the brightness without invoking significant dissociative excitation of molecules. Surprisingly, the nonresponse of O and rapid depletion of Na is opposite the temporal behavior of their SO 2 and NaCl parent molecules during Io’s eclipse phase.
Article
Full-text available
In this work, we present the most updated catalog of Io hot spots based on Juno/JIRAM data. We find 242 hot spots, including 23 previously undetected. Over the half of the new hot spots identified, are located at high northern and southern latitudes (>70°). We observe a latitudinal variability and a larger concentration of hot spots in the polar regions, in particular in the North. The comparison between JIRAM and the most recent Io hot spot catalogs listing power output (Veeder et al., 2015, https://doi.org/10.1016/j.icarus.2014.07.028; de Kleer, de Pater, et al., 2019, https://doi.org/10.3847/1538-3881/ab2380), shows JIRAM detected 63% and 88% of the total number of hot spots, respectively. Furthermore, JIRAM observed 16 of the 34 faint hot spots previously identified. JIRAM data revealed thermal emission from 5 dark pateræ inferred to be active from color ratio images, thus confirming that these are hot spots.
Article
Full-text available
We collected a set of published, higher-order data products of Jupiter's volcanic moon Io and assembled them in an ArcGIS tm database we are calling the Io GIS Database, version 1.0. The purpose of this database is to collect image, topographic, geologic, and thermal emission data of Io in one geospatially registered location to form the data component of an Io planetary spatial data infrastructure (PSDI). The goals of an Io PSDI are (1) to make higher-order data products more accessible and usable to the broader planetary science community, particularly to new scientists that were not associated with the projects that obtained the data; (2) to enable new scientific studies with the data; and (3) to create a tool to support observation planning for future Io-focused planetary missions. In this paper we describe the motivation behind our project, discuss the data sets acquired for this first version of the database, and demonstrate how they can be used. We conclude with a discussion of how our database relates to other PSDIs, our plans for future updates, and a request for additional Io data sets.
Article
The Archean continents, primarily composed of the felsic tonalite–trondhjemite–granodiorite (TTG) suite, were formed or conserved since ~ 3.8 Ga, with significant growth of the continental crust since ~ 2.7 Ga. The difficulty in direct differentiation of the felsic crustal components from Earth’s mantle peridotite leads to a requirement for the presence of a large amount of hydrated mafic precursor of TTG in Earth’s proto-crust, the origin of which, however, remains elusive. The mafic proto-crust may have formed as early as ~ 4.4 Ga ago as reflected by the Hf and Nd isotopic signals from Earth’s oldest geological records. Such a significant time lag between the formation of the mafic proto-crust and the occurrence of felsic continental crust is not reconciled with a single-stage scenario of Earth’s early differentiation. Here, inspired by the volcanism-dominated heat-pipe tectonics witnessed on Jupiter’s moon Io and the resemblances of the intensive internal heating and active magmatism between the early Earth and the present-day Io, we present a conceptual model of Earth’s early crust-mantle differentiation, which involves an Io-like scenario of efficient extraction of a mafic proto-crust from the early mantle, followed by an intrusion-dominating regime that could account for the subsequent formation of the felsic continents as Earth cools. The model thus allows an early formation of the pre-TTG proto-crust and the generation of TTG in the continent by providing the favorable conditions for its subsequent melting. This model is consistent with the observed early fractionation of the Earth and the late but rapid formation and/or accumulation of the felsic components in the Archean continents, thus sheds new light on the early Earth’s differentiation and tectonic evolution.
Article
Full-text available
Jupiter’s aurora features have been observed by the Hubble space telescope (HST) for over two decades. One of the auroral features, Ganymede’s magnetic footprint, appears close to the main emission and is sometimes embedded in the main emission. The latter case causes difficulty in identifying Ganymede’s magnetic footprint from in the main emission. The FUV aurora images were taken by Advanced Camera for Surveys (ACS) onboard the HST. The fluctuations of Ganymede’s footprint brightness over time will be analyzed. Moreover, the correlation between the brightness and locations of the main emission and Ganymede’s magnetic footprint will be analyzed to characterize the connection between ionospheric phenomena and the magnetospheric dynamics. Since the main emission is very bright in comparison with the footprint, therefore, the variation of the main emission can affect the Ganymede’s magnetic footprint. Furthermore, the expansion of the main emission is consistent with the location shift of Ganymede’s magnetic footprint in equatorward direction. The brightness and location of the main emission can be influenced by the plasma variation in Jupiter’s magnetosphere which is affected partly by the volcanic eruption on Io and solar wind dynamic pressure. The variation of Ganymede magnetic footprint’s brightness and location in respond to the main emission could be an important indicator of the magnetospheric variation under the influences of internal and external factors.
Preprint
Full-text available
A geometric technique is introduced to estimate the height of volcanic eruption columns using the generally discarded near-limb portion of geostationary imagery. Such oblique observations facilitate a height-by-angle estimation method by offering close to orthogonal side views of eruption columns protruding from the Earth ellipsoid. Coverage is restricted to daytime point estimates in the immediate vicinity of the vent, which nevertheless can provide complementary constraints on source conditions for the modelling of near-field plume evolution. The technique is best suited to strong eruption columns with minimal tilting in the radial direction. For weak eruptions with severely bent plumes or eruptions with expanded umbrella clouds the radial tilt/expansion has to be corrected for either visually or using ancillary wind profiles. Validation on a large set of mountain peaks indicates a typical height uncertainty of ±500 m for near-vertical eruption columns, which compares favourably with the accuracy of the common temperature method.
Article
Full-text available
Volcanic plumes on Jupiter's moon Io are modeled using the direct simulation Monte Carlo (DSMC) method. The modeled volcanic vent is interpreted as a “virtual” vent. A parametric study of the “virtual” vent gas temperature and velocity is performed to constrain the gas properties at the vent by observables, particularly the plume height and the surrounding condensate deposition ring radius. Also, the flow of refractory nano-size particulates entrained in the gas is modeled with “overlay” techniques which assume that the background gas flow is not altered by the particulates. The column density along the tangential line-of-sight and the shadow cast by the plume are calculated and compared with Voyager and Galileo images. The parametric study indicates that it is possible to obtain a unique solution for the vent temperature and velocity for a large plume like Pele. However, for a small Prometheus-type plume, several different possible combinations of vent temperature and velocity result in both the same shock height and peak deposition ring radius. Pele and Prometheus plume particulates are examined in detail. Encouraging matches with observations are obtained for each plume by varying both the gas and particle parameters. The calculated tangential gas column density of Pele agrees with that obtained from HST observations. An upper limit on the size of particles that track the gas flow well is found to be ∼10 nm, consistent with Voyager observations of Loki. While it is certainly possible for the plumes to contain refractory dust or pyroclastic particles, especially in the vent vicinity, we find that the conditions are favorable for SO2 condensation into particles away from the vent vicinity for Prometheus. The shadow cast by Prometheus as seen in Galileo images is also reproduced by our simulation. A time averaged frost deposition profile is calculated for Prometheus in an effort to explain the multiple ring structure observed around the source region. However, this multiple ring structure may be better explained by the calculated deposition of entrained particles. The possibility of forming a dust cloud on Io is examined and, based on a lack of any such observed clouds, a subsolar frost temperature of less than 118 K is suggested.
Article
Infrared wavelength observations of Io by the Galileo spacecraft show that at least 12 different vents are erupting lavas that are probably hotter than the highest temperature basaltic eruptions on Earth today. In at least one case, the eruption near Pillan Patera, two independent instruments on Galileo show that the lava temperature must have exceeded 1700 kelvin and may have reached 2000 kelvin. The most likely explanation is that these lavas are ultramafic (magnesium-rich) silicates, and this idea is supported by the tentative identification of magnesium-rich orthopyroxene in lava flows associated with these high-temperature hot spots.
Article
Pele and Pillan Patera are volcanoes on Io. Analysis of Galileo NIMS and SSI data has allowed the modeling of the eruptions at these two sites. Pele appears to be a disrupted lava lake. Pillan Patera is the site of a massive (though brief) eruption.
Article
We report adaptive optics observations of Io from 17th April and 1st, 2nd of June 2006 (UT), taken using the near-infrared imaging spectrometer, OSIRIS, on the 10m W.M. Keck II telescope. We obtained z(980-1199nm), J(1180-1440nm), H(1473-1803nm), K(1965-2381nm) broadband spectral cube mosaics of Io's entire disk with a 0.02'' plate-scale and multiple K broadband cubes using the 0.05'' plate-scale. On the 17th April and 2nd of June we observed a bright outburst in Io's northern hemisphere, which we provisionally attribute to the Tvashtar Catena. The eruption flux was strongest in the K band and initial analysis of the broadband J, H and K band spectra imply a temperature of 1150-1250K. Current analysis involves a multi-temperature blackbody fit and photometric flux calibration to estimate the area covered by the eruption. This research is supported by NSF grant AST-0406275 and via CfAO's cooperative agreement AST-9876783.
Article
Ground-based observations of volcanism on Io during the period of the 1999 and early 2000 Galileo close flybys have detected several types of activity, providing information which complements the spacecraft observations. At Loki a brightening began between August 25 and September 9 and continued through February. On August 2 a major outburst was observed near (14°N, 74°W) whose brightness corresponds to an area of approximately 350 km2 at a temperature of 1100 K. Observations of eruptions in late June (9906A) and in late November (9911A, at Tvashtar) provide temporal and photometric constraints on activity also seen by Galileo. High-resolution adaptive optics images provide further information on the fainter sources distributed across the surface.
Article
Clear-filter imaging of Io during the Galileo nominal and extended missions recorded diffuse auroral emissions in 16 distinct observations taken during 14 separate eclipses over a two year period. These images show that the morphology and time variability of the visible aurora have several similarities to Io's far ultraviolet emissions. The orbital leading hemisphere of Io is consistently brighter than the trailing hemisphere, probably due to a greater concentration of torus electrons in the wake region of the satellite. The locations of the polar limb glow and the bright equatorial glows appear to correlate with Io's System III longitude. Unlike the far ultraviolet emissions, the visible aurorae are enhanced near actively venting volcanic plumes, probably because of molecular emission by SO2.
Article
We present in this Keck AO paper the first global high angular resolution observations of Io in three broadband near-infrared filters: Kc (2.3 μm), Lp (3.8 μm), and Ms (4.7 μm). The Keck AO observations are composed of 13 data sets taken during short time intervals spanning 10 nights in December, 2001. The MISTRAL deconvolution process, which is specifically aimed for planetary images, was applied to each image. The spatial resolution achieved with those ground-based observations is 150, 240, and 300 km in the Kc, Lp, and Ms band, respectively, making them similar in quality to most of the distant observations of the Galileo/NIMS instrument. Eleven images per filter were selected and stitched together after being deprojected to build a cylindrical map of the entire surface of the satellite. In Kc-band, surface albedo features, such as paterae (R>60 km) are easily identifiable. The Babbar region is characterized by extremely low albedo at 2.2 μm, and shows an absorption band at 0.9 μm in Galileo/SSI data. These suggest that this region is covered by dark silicate deposits, possibly made of orthopyroxene. In the Lp–Ms (3–5 μm) bands, the thermal emission from active centers is easily identified. We detected 26 hot spots in both broadband filters over the entire surface of the minor planet; two have never been seen active before, nine more are seen in the Ms band. We focused our study on the hot spots detected in both broadband filters. Using the measurements of their brightness, we derived the temperature and area covered by 100 brightness measurements. Loki displayed a relatively quiescent activity. Dazhbog, a new eruption detected by Galileo/NIMS in August 2001, is a major feature in our survey. We also point out the fading of Tvashtar volcanic activity after more than two years of energetic activity, and the presence of a hot, but small, active center at the location of Surt, possibly a remnant of its exceptional eruption detected in February 2001. Two new active centers, labeled F and V on our data, are detected. Using the best temperature and the surface area derived from the L and M band intensities, we calculated the thermal output of each active center. The most energetic hot spots are Loki and Dazhbog, representing respectively 36 and 19% of the total output calculated from a temperature fit of all hot spots (20.6×1012 W). Based on the temperature derived from hot spots (∼400 K), our measurement can unambiguously identify the contribution to the heat flux from the silicate portion of the surface. Because the entire surface was observed, no extrapolation was required to calculate that flux. It is also important to note that we measured the brightness of the individual hot spots when they were located close to the Central Meridian. This minimizes the line-of-sight effect which does not follow strictly a classical cosine law. Finally, we argue that despite the widespread volcanic activity detected, Io was relatively quiescent in December 2001, with a minimum mean total output of 0.4–1.2 W m−2. This output is at least a factor of two lower than those inferred from observations made at longer wavelengths and at different epochs.
Article
Active volcanism on Io has been monitored during the nominal Galileo satellite tour from mid 1996 through late 1997. The Solid State Imaging (SSI) experiment was able to observe many manifestations of this active volcanism, including (1) changes in the color and albedo of the surface, (2) active airborne plumes, and (3) glowing vents seen in eclipse.About 30 large-scale (tens of kilometers) surface changes are obvious from comparison of the SSI images to those acquired by Voyager in 1979. These include new pyroclastic deposits of several colors, bright and dark flows, and caldera-floor materials. There have also been significant surface changes on Io during the Galileo mission itself, such as a new 400-km-diameter dark pyroclastic deposit around Pillan Patera. While these surface changes are impressive, the number of large-scale changes observed in the four months between the Voyager 1 and Voyager 2 flybys in 1979 suggested that over 17 years the cumulative changes would have been much more impressive. There are two reasons why this was not actually the case. First, it appears that the most widespread plume deposits are ephemeral and seem to disappear within a few years. Second, it appears that a large fraction of the volcanic activity is confined to repeated resurfacing of dark calderas and flow fields that cover only a few percent of Io's surface.The plume monitoring has revealed 10 active plumes, comparable to the 9 plumes observed by Voyager. One of these plumes was visible only in the first orbit and three became active in the later orbits. Only the Prometheus plume has been consistently active and easy to detect. Observations of the Pele plume have been particularly intriguing since it was detected only once by SSI, despite repeated attempts, but has been detected several times by the Hubble Space Telescope at 255 nm. Pele's plume is much taller (460 km) than during Voyager 1 (300 km) and much fainter at visible wavelengths. Prometheus-type plumes (50–150 km high, long-lived, associated with high-temperature hot spots) may result from silicate lava flows or shallow intrusions interacting with near-surface SO2.A major and surprising result is that ∼30 of Io's volcanic vents glow in the dark at the short wavelengths of SSI. These are probably due to thermal emission from surfaces hotter than 700 K (with most hotter than 1000 K), well above the temperature of pure sulfur volcanism. Active silicate volcanism appears ubiquitous. There are also widespread diffuse glows seen in eclipse, related to the interaction of energetic particles with the atmosphere. These diffuse glows are closely associated with the most active volcanic vents, supporting suggestions that Io's atmopshere is dominated by volcanic outgassing.Globally, volcanic centers are rather evenly distributed. However, 14 of the 15 active plumes seen by Voyager and/or Galileo are within 30° of the equator, and there are concentrations of glows seen in eclipse at both the sub- and antijovian points. These patterns might be related to asthenospheric tidal heating or tidal stresses. Io will continue to be observed during the Galileo Europa Mission, which will climax with two close flybys of Io in late 1999.
Article
Io, the innermost Galilean satellite of Jupiter, is a fascinating world. Data taken by Voyager and Galileo instruments have established that it is by far the most volcanic body in the Solar System and suggest that the nature of this volcanism could radically differ from volcanism on Earth. We report on near-IR observations taken in February 2001 from the Earth-based 10-m W. M. Keck II telescope using its adaptive optics system. After application of an appropriate deconvolution technique (MISTRAL), the resolution, ∼100 km on Io's disk, compares well with the best Galileo/NIMS resolution for global imaging and allows us for the first time to investigate the very nature of individual eruptions. On 19 February, we detected two volcanoes, Amirani and Tvashtar, with temperatures differing from the Galileo observations. On 20 February, we noticed a slight brightening near the Surt volcano. Two days later it had turned into an extremely bright volcanic outburst. The hot spot temperatures (>1400 K) are consistent with a basaltic eruption and, being lower limits, do not exclude an ultramafic eruption. These outburst data have been fitted with a silicate-cooling model, which indicates that this is a highly vigorous eruption with a highly dynamic emplacement mechanism, akin to fire-fountaining. Its integrated thermal output was close to the total estimated output of Io, making this the largest ionian thermal outburst yet witnessed.