These two global images of Iapetus show the extreme brightness dichotomy on
the surface of this peculiar Saturnian moon. The left-hand panel shows the
moon's leading hemisphere and the right-hand panel shows the moon's trailing
side. While low and mid latitudes of the leading side exhibit a surface almost
as dark as charcoal, broad tracts of the trailing side are almost as bright as
snow. The dark terrain covers about 40 percent of the surface and is named
Cassini Regio. The names of the bright terrain are Roncevaux Terra (north) and
Saragossa Terra (south).
On both hemispheres, the dominant landforms are
impact craters. The largest known well-preserved basin on Iapetus, called
Turgis, has a diameter of about 580 kilometers (360 miles). It lies at 17
degrees north latitude, 28 degrees west longitude at the eastern edge of the
dark Cassini Regio and is visible on the right side of the left-hand panel. The
prominent basin on the southern trailing side (at the lower left of the
right-hand panel) is Engelier. Engelier is located at 41 degrees south latitude,
265 degrees west longitude, and has a diameter of about 504 kilometers (313
miles). Its formation destroyed about half of Gerin, another large basin on
Iapetus. Gerin is located at 46 degrees south latitude, 233 degrees west
longitude, and has a diameter of about 445 kilometers (276 miles). Tortelosa
Montes, a part of the giant equatorial ridge that was discovered in Cassini
images on December 25, 2004, is visible in the left panel as a thin line within
Cassini Regio, and as a tall prominence at the western limb. It continues onto
the trailing side (right side of right panel), where the bright western flanks
of the Carcassone Montes appear as dominant bright spots within the western edge
of Cassini Regio.
The cause of the extreme brightness dichotomy on
Iapetus is likely to be thermal segregation of water ice on a global scale.
Thermal effects are usually expected to act latitudinally. That is, polar areas
are colder than equatorial terrain in most cases due to the more oblique angle
of the solar irradiation. Therefore, an additional process is required to
explain the longitudinal difference as well. In one model, dark, reddish dust
coming in from space and preferentially deposited on the leading side forms a
small, but crucial difference between the leading and trailing hemispheres,
which is sufficient to allow the thermal effect to evaporate the water ice on
the leading side completely, but only marginally on the trailing side.
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