posted on 2017-01-04, 09:51authored byLeigh N. Fletcher, G. S. Orton, J. H. Rogers, R. S. Giles, A. V. Payne, P. G. J. Irwin, M. Vedovato
The transformation of Jupiter’s South Equatorial Belt (SEB) from its faded, whitened state in 2009-2010 (Fletcher et al., 2011b)
to its normal brown appearance is documented via comparisons of thermal-infrared (5-20 µm) and visible-light imaging between
November 2010 and November 2011. The SEB revival consisted of convective eruptions triggered over ∼ 100 days, potentially
powered by the latent heat released by the condensation of water. The plumes rise from the water cloud base and ultimately diverge
and cool in the stably-stratified upper troposphere. Thermal-IR images from the Very Large Telescope (VLT) were acquired 2 days
after the SEB disturbance was first detected as a small white spot by amateur observers on November 9th 2010. Subsequent images
over several months revealed the cold, putatively anticyclonic and cloudy plume tops (area 2.5 × 106 km2
) surrounded by warm,
cloud-free conditions at their peripheries due to subsidence. The latent heating was not directly detectable in the 5-20 µm range. The
majority of the plumes erupted from a single source near 140−160◦W, coincident with the remnant cyclonic circulation of a brown
barge that had formed during the fade. The warm remnant of the cyclone could still be observed in IRTF imaging 5 days before
the November 9th eruption. Additional plumes erupted from the leading edge of the central disturbance immediately east of the
source, which propagated slowly eastwards to encounter the Great Red Spot. The tropospheric plumes were sufficiently vigorous to
excite stratospheric thermal waves over the SEB with a 20−30◦
longitudinal wavelength and 5-6 K temperature contrasts at 5 mbar,
showing a direct connection between moist convection and stratospheric wave activity. The subsidence and compressional heating
of dry, unsaturated air warmed the troposphere (particularly to the northwest of the central branch of the revival) and removed the
aerosols that had been responsible for the fade. Dark, cloud-free lanes west of the plumes were the first to show the colour change,
and elongated due to the zonal windshear to form the characteristic ‘S-shape’ of the revival complex. The aerosol-free air was
redistributed and mixed throughout the SEB by the zonal flow, following a westward-moving southern branch and an eastwardmoving
northern branch that revived the brown colouration over ∼ 200 days. The transition from the cool conditions of the SEBZ
during the fade to the revived SEB caused a 2-4 K rise in 500-mbar temperatures (leaving a particularly warm southern SEB) and
a reduction of aerosol opacity by factors of 2-3. Newly-cleared gaps in the upper tropospheric aerosol layer appeared different in
filters sensing the ∼ 700-mbar cloud deck and the 2-3 bar cloud deck, suggesting complex vertical structure in the downdrafts. The
last stage of the revival was the re-establishment of normal convective activity northwest of the GRS in September 2011, ∼ 840
days after the last occurrence in June 2009. Moist convection may therefore play an important role in controlling the timescale and
atmospheric variability during the SEB life cycle.
Funding
Fletcher was supported by a Royal Society Research Fellowship
at the University of Leicester, Giles was supported by a
Royal Society research grant at the University of Oxford. The
UK authors acknowledge the support of the Science and Technology
Facilities Council (STFC). A portion of this work was
performed by Orton and Payne at the Jet Propulsion Laboratory,
California Institute of Technology, under a contract with
NASA. This research used the ALICE High Performance Computing
Facility at the University of Leicester. We are extremely
grateful for the combined efforts of the numerous amateur observers
(including those listed in the figure captions) for sharing
their data, and for the JUPOS software developed by Grischa
Hahn and Hans-Jorg Mettig to reproject the visible-light data. ¨
This investigation was partially based on thermal-infrared
observations acquired at (i) the ESO Very Large Telescope
Paranal UT3/Melipal Observatory using Directors Discretionary
Time (program ID 286.C-5009) and regular service time
(program ID 087.C-0024); (ii) the Subaru Telescope, which is
27
operated by the National Astronomical Observatory of Japan
(program ID O11154); (iii) NASA’s Infrared Telescope Facility,
which is operated by the University of Hawaii under contract
NNH14CK55B with the National Aeronautics and Space Administration
(program IDs 2010B010, 2011A010, 2011B027);
and (iv) observations obtained at the Gemini Observatory (program
IDs GN-2010B-DD-3, GS-2010B-Q-8 and GS-2011AQ-11),
which is operated by the Association of Universities
for Research in Astronomy, Inc., under a cooperative agreement
with the NSF on behalf of the Gemini partnership: the
National Science Foundation (United States), the National Research
Council (Canada), CONICYT (Chile), Ministerio de
Ciencia, Tecnolog´ıa e Innovacion Productiva (Argentina), and ´
Ministerio da Ci ´ encia, Tecnologia e Inovac¸ ˆ ao (Brazil). We wish ˜
to recognise and acknowledge the very signif
History
Citation
Icarus 2017, 286, pp. 94–117
Author affiliation
/Organisation/COLLEGE OF SCIENCE AND ENGINEERING/Department of Physics and Astronomy