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Iapetus' geophysics: Rotation rate, shape, and equatorial ridge
Authors:J.C. Castillo-Rogez  D.L. Matson  T.V. Johnson  P.C. Thomas
Affiliation:a Jet Propulsion Laboratory, California Institute of Technology, M/S 230-260, 4800 Oak Grove Drive, Pasadena, CA 91109, USA
b UMR - CNRS 6112 Laboratoire de planétologie et géodynamique de Nantes, 2, rue de la Houssinière, 44322 Nantes Cedex 3, France
c Lunar and Planetary Laboratory, 1629 E. University Blvd., Tucson, AZ 85721-0092, USA
d Department of Astronomy, Cornell University, 422 Space Sciences Building, Ithaca, NY 14853, USA
Abstract:Iapetus has preserved evidence that constrains the modeling of its geophysical history from the time of its accretion until now. The evidence is (a) its present 79.33-day rotation or spin rate, (b) its shape that corresponds to the equilibrium figure for a hydrostatic body rotating with a period of ∼16 h, and (c) its high, equatorial ridge, which is unique in the Solar System. This paper reports the results of an investigation into the coupling between Iapetus' thermal and orbital evolution for a wide range of conditions including the spatial distributions with time of composition, porosity, short-lived radioactive isotopes (SLRI), and temperature. The thermal model uses conductive heat transfer with temperature-dependent conductivity. Only models with a thick lithosphere and an interior viscosity in the range of about the water ice melting point can explain the observed shape. Short-lived radioactive isotopes provide the heat needed to decrease porosity in Iapetus' early history. This increases thermal conductivity and allows the development of the strong lithosphere that is required to preserve the 16-h rotational shape and the high vertical relief of the topography. Long-lived radioactive isotopes and SLRI raise internal temperatures high enough that significant tidal dissipation can start, and despin Iapetus to synchronous rotation. This occurred several hundred million years after Iapetus formed. The models also constrain the time when Iapetus formed because the successful models are critically dependent upon having just the right amount of heat added by SLRI decay in this early period. The amount of heat available from short-lived radioactivity is not a free parameter but is fixed by the time when Iapetus accreted, by the canonical concentration of 26Al, and, to a lesser extent, by the concentration of 60Fe. The needed amount of heat is available only if Iapetus accreted between 2.5 and 5.0 Myr after the formation of the calcium aluminum inclusions as found in meteorites. Models with these features allow us to explain Iapetus' present synchronous rotation, its fossil 16-h shape, and the context within which the equatorial ridge arose.
Keywords:Iapetus   Interiors   Geophysics   Satellites, shapes   Satellites, dynamics
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