Cratering rates on synchronously
rotating satellites
Kevin Zahnle and Paul
Schenk
Impact cratering of synchronously-rotating
satellites is expected to occur faster on the leading hemisphere than on the
trailing hemisphere. This occurs because the satellite’s orbital velocity around
the planet is generally large compared to the space velocities of comets and
asteroids. The relationship between comets and moons is broadly akin to that
between flies and windshields. As it is with cars, the predicted asymmetry is
large, with cratering rates at the apex of motion (the center of the leading
hemisphere) typically 30-80 times greater than at the antapex. However, the
expected asymmetry is at best poorly expressed on actual satellites, with the
alarming exception of Triton, where the observed asymmetry is apparently too
great. The failure to observe the seemingly inevitable suggests that some of
these satellites have led, and may still be leading, interesting lives.
This study used a suite
of Monte Carlo simulations to better determine how cratering rates vary across
the surfaces of synchronous satellites. The method generates orbits randomly
from ancestral distributions that arguably are isotropic, or nearly so; assign
to each orbit an impact probability and to each a possible impact site and appropriate
crater diameter; while also allowing practical treatment of many effects that
would be dauntingly difficult to treat analytically. An empirical fit to the
suite of numerical experiments is that the cratering rate
,
where
refers to the circular orbital velocity of the satellite and
refers to the characteristic encounter velocity of the ecliptic comet with the
planet; the angle b is the angular distance measured from the apex of motion;
and the parameter g is the power law exponent describing the assumed cumulative
size distribution of the impactors,
,
where d is diameter. The expression works well for 1<g<4; real
solar system populations typically have 1.5<g<3.
As noted above, the predicted
cratering asymmetries are not seen in fact. Most synchronous satellites are
effectively saturated with impact craters, for which no signature of a leading/trailing
cratering asymmetry is to be expected. The three interesting exceptions are
Ganymede and Europa, moons of Jupiter, and Triton, chief moon of Neptune. Europa
has few impact craters and no obvious leading/trailing asymmetry. But this is
not surprising, because Europa’s icy shell is decoupled from the interior by
a liquid water ocean: it would be relatively easy for the shell to rotate nonsynchronously.
Ganymede is a more interesting case. Careful analysis reveals that Ganymede
does preserve a fourfold asymmetry between fore and aft. This is much less than
the 60-fold asymmetry expected but in the right direction; a possible interpretation
is that Ganymede once rotated nonsynchronously but does so no longer. This in
turn implicates a once thicker liquid water ocean for Ganymede, a conclusion
in harmony with other clues that Ganymede was once much more like Europa than
it is now.
Finally, there is Triton.
Triton revolves in a retrograde orbit around Neptune. It appears to be a captured
comet that melted as its orbit tidally evolved from a highly eccentric ellipse
to a circle. Triton has very few craters. Its surface is obviously geologically
young, probably no older than Europa’s. Essentially all of its impact craters
are on its leading hemisphere. In particular, a lack of craters near b=90° appears
to be real, as this region (facing Neptune) was the part of Triton seen best
by the Voyager 2 spacecraft. This cratering pattern is too asymmetric
to be accounted for by comets or other objects that orbit the sun. Required
rather are objects in prograde orbit around Neptune. Such objects would strike
Triton mostly head-on, and the resulting craters would be mostly confined to
the leading hemisphere. The origin of the implied swarm of prograde, Neptune-orbiting
debris is an open question. The alternative explanation is that Triton has been
capriciously resurfaced so as to look to us, from the one viewpoint of the Voyager
2, as if it had run face-first into a swarm of debris.