B. Bezard et al., THERMAL INFRARED IMAGING SPECTROSCOPY OF SHOEMAKER-LEVY-9 IMPACT SITES - TEMPERATURE AND HCN RETRIEVALS, Icarus, 125(1), 1997, pp. 94-120
We present high-resolution 8-14 mu m observations of Shoemaker-levy 9
sites conducted on July 20, 30, and 31 1994 UT at the NASA Infrared Te
lescope Facility. Stratospheric heating was detected from strong enhan
cements of methane emission near 8.1 mu m over areas at least 15,000 k
m wide around the K site observed 23 hr after impact and around the L
site 11 hr after impact. The intensity distribution between strong and
weaker CH4 lines implies that the stratospheric heating was primarily
confined to pressures less than 500 mu bar. The L site temperature in
creased by 80 +/- 10 K at 5 mu bar, but did not exceed 20 K around 1 m
bar or 10 K around 10 mbar. The older K site was still 30 +/- 5 K warm
er than the surroundings at the 10-mu bar level. The excess thermal en
ergy stored in the upper jovian stratosphere was 3(-1.5)(+3) x 10(26)
erg over the L site, and 2(-1)(+2) x 10(26) erg over the K site at the
time of the observations. Comparison with numerical simulations indic
ates that a large fraction (>20%) of the kinetic energy of the L plume
was transferred to the jovian atmosphere and not immediately radiated
away. Acetylene line emission near 13.4 mu m was enhanced over an are
a similar to 18,000 km wide centered on the E site 2.6 days after impa
ct. Radiative transfer models of this emission indicate temperatures 3
7 +/- 7 K higher than nominal around 3 mu bar. No such enhancement was
seen in CH, spectral images, implying that the temperature perturbati
on did not significantly extend below the similar to 20-mu bar level.
The H site observed simultaneously was 12 +/- 5 K warmer than the surr
oundings 1.4 day after impact. C2H2 lines were still slightly more int
ense over the K + W and Q1 sites on July 30 and 31, 8 to 10 days after
impact. These observations can be interpreted either by temperature d
ifferences of about 13 and 10 K respectively in the 3-mu bar region, o
r by an increase in the C2H2 column density of 2.5-5 x 10(17) molecule
cm(-2). Emission from hydrogen cyanide lines around 13.4 mu m was det
ected over all sites observed, The mass of HCN is about 2 x 10(12) g f
or the biggest plumes (K, L, G), 0.95 +/- 0.5 x 10(12) g over the E si
te, and 0.45 +/- 0.2 x 10(12) g over the H site, The total mass of HCN
produced by all fragments is estimated to be 1.1 +/- 0.4 x 10(13) g.
A consistent interpretation of the different pieces of information ava
ilable suggests that the H plume was richer in dust than the E or A pl
ume. (C) 1997 Academic Press