Author/Authors :
Deau، نويسنده , , Estelle and Dones، نويسنده , , Luke and Rodriguez، نويسنده , , Sébastien and Charnoz، نويسنده , , Sébastien and Brahic، نويسنده , , André، نويسنده ,
Abstract :
In this paper, we characterize the morphology of the disk-integrated phase functions of satellites and rings around the giant planets of our solar system. We find that the shape of the phase function is accurately represented by a logarithmic model [Bobrov, M.S., 1970. Physical properties of Saturnʹs rings. In: Dollfus, A. (Ed.), Surfaces and Interiors of Planets and Satellites. Academic, New York, pp. 376–461]. For practical purposes, we also parametrize the phase curves by a linear-exponential model [Kaasalainen, S., Muinonen, K., Piironen, J., 2001. Comparative study on opposition effect of icy solar system objects. Journal of Quantitative Spectroscopy and Radiative Transfer 70, 529–543] and a simple linear-by-parts model [Lumme, K., Irvine, W.M., 1976. Photometry of Saturnʹs rings. Astronomical Journal 81, 865–893], which provides three morphological parameters: the amplitude A and the half-width at half-maximum (HWHM) of the opposition surge, and the slope S of the linear part of the phase function at larger phase angles.
alysis demonstrates that all of these morphological parameters are correlated with the single-scattering albedos of the surfaces.
ing more accurately into consideration the finite angular size of the Sun, we find that the Galilean, Saturnian, Uranian and Neptunian satellites have similar HWHMs ( ≲ 0 . 5 ∘ ), whereas they have a wide range of amplitudes A. The Moon has the largest HWHM ( ∼ 2 ∘ ). We interpret that as a consequence of the “solar size bias”, via the finite angular size of the Sun which varies dramatically from the Earth to Neptune. By applying a new method that attempts to morphologically deconvolve the phase function to the solar angular size, we find that icy and young surfaces, with active resurfacing, have the smallest values of A and HWHM, whereas dark objects (and perhaps older surfaces) such as the Moon, Nereid and Saturnʹs C ring have the largest A and HWHM.
ison between multiple objects also shows that solar system objects belonging to the same planet have comparable opposition surges. This can be interpreted as a “planetary environmental effect” that acts to locally modify the regolith and the surface properties of objects which are in the same environment.
Keywords :
Planetary rings , opposition effect , Satellites of Jupiter , coherent-backscattering and shadow-hiding , Uranus , phase curves , angular size of the solar radius , Neptune , Saturn