Jl. Ortiz et al., THE SHOEMAKER-LEVY-9 H-IMPACT - SOME RESULTS FROM THE WILLIAM-HERSCHEL TELESCOPE, Astronomy and astrophysics, 324(1), 1997, pp. 357-365
We present a CCD lightcurve for the H impact observed at 948 nm by the
4.2-m William Herscher Telescope at La Palma (Spain). We compare the
results with other lightcurves at visible and near infrared. There app
ears to be a common pattern in all the CCD lightcurves: An initial rel
ative maximum is followed by a relative minimum and another maximum. C
onsidering the plume as a superposition of material ejected at various
speeds, we suggest the first maximum is likely due to reflected solar
light by the plume at its widest phase. The minimum may be due to the
disappearance of part of the plume, as the material ejected with vert
ical velocities lower than 9 km/s descends in its ballistic trajectory
and penetrates below the level of solar illumination. The following m
aximum is most likely due to thermal emission from the reimpacting eje
cta (either from the particulates or the gas). The timing of the secon
d maximum and the moment of detection of the plume suggest vertical ve
locities in the range 9-12 km/s for most of the ejecta, with peak part
icle concentration at 11 km/s for the L impact, according to our inter
pretation of Schleicher et al. (1994) lightcurve. The atmospheric leve
l where the visible emission takes place is estimated to be P = 25(-25
)(+65) mbar and P = 35(-35)(+30) mbar for the L and H impacts, respect
ively.