Radiogenic heating of comets by 26Al and implications for their time of formation.
The effect of radiogenic heating on the thermal evolution of spherical icy bodies with radii 1 km < R < 100 km was investigated.  The radioisotopes considered were 26Al, 40K, 232Th, 235U, and 238U.  Except for the 26Al abundance, which was varied, the other initial abundances were kept fixed, at values derived from those of chondritic meteorites and corresponding to a gas-to-dust ratio of 1.  The initial models were homogeneous and isothermal (To = 10 K) amorphous ice spheres, in a circular orbit at 10(4) AU from the Sun.  The main object of this study was to examine the conditions under which the transition temperature from amorphous into cubic ice (Ta = 137 K) would be reached.  It was shown that the influence of the short-lived radionuclide 26Al dominates the effect of other radioactive species for bodies of radii up to approximately 50 km.  Consequently, if we require comets to retain their ice in amorphous form, as suggested by observations, an upper limit of approximately 4 x 10(-9) is obtained for the initial 26Al abundance in comets, a factor of 100 lower than that of the inclusions in the Allende meteorite.  A lower limit for the formation time of comets may thus be derived.  The possibility of a coexistence of molten cometary cores and extended amorphous ice mantles is ruled out.  Larger icy spheres (R > 100 km) reached Ta even in the absence of 26Al, due to the decay of the other radionuclides.  As a result, a crystalline core formed whose relative size depended on the composition assumed.  Thus the outermost icy satellites in the solar system, which might have been formed of ice in the amorphous state, have probably undergone crystallization and may have exhibited eruptive activity when the gas trapped in the amorphous ice was released (e.g., Miranda).
Prialnik
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D
Department of Geophysics and Planetary Sciences, Tel Aviv University.
Bar-Nun
A
A
Podolak
M
M
D000535:Aluminum; D055580:Astronomical Phenomena; D001256:Astronomy; D003460:Crystallization; D006358:Hot Temperature; D007053:Ice / Q000032:analysis*; D008433:Mathematics; D019110:Meteoroids; D008962:Models, Theoretical; D011851:Radioactivity; D011868:Radioisotopes; D013057:Spectrum Analysis
D007053:Ice; D011868:Radioisotopes; D000535:Aluminum