K. Hashizume et N. Sugiura, TRANSPORTATION OF GASEOUS ELEMENTS AND ISOTOPES IN A THERMALLY EVOLVING CHONDRITIC PLANETESIMAL, Meteoritics & planetary science, 33(5), 1998, pp. 1181-1195
The behavior of H, C, N and their isotopes in a thermally evolving pla
netesimal was evaluated by numerical simulation. Transportation of hea
t and gas molecules, and the chemical equilibrium involving these elem
ents, were simulated. Our modeled planetesimals initially contain homo
geneous amounts of radioactive heat source (Al-26); and H, C, and N in
forms of organic materials, graphite, and in some models, water ice.
Vaporized gas molecules were transported from the interior of the plan
etesimal to its surface, although their transportation efficiencies we
re quite different among the three elements, primarily due to differen
ces in their affinities to metallic Fe. Significant portions of these
elements were redistributed into metallic Fe when the planetesimal was
heated at 600 degrees C and above. Nitrogen showed the most prominent
siderophile characteristics, resulting in fairly large concentrations
of N trapped in metallic Fe, which is consistent with observations by
Hashizume and Sugiura (1997). Efficiency of C transportation cruciall
y depended on O fugacity. To realize effective C transportation, it wa
s necessary to assume an oxidizing condition (log fO(2) > log fO(2,(FI
F)) + 1) in the initially accreted material. Water vapor, generated at
the interior of the planetesimal and transported to its near surface,
formed a water-rich layer under certain conditions, providing an envi
ronment sufficient for aqueous alteration of chondritic materials to o
ccur. Variations in isotopic ratios of N in taenite observed among equ
ilibrated ordinary chondrites can be explained by our gas transportati
on model. It is required, however, that carriers of isotopically anoma
lous N, perhaps presolar grains, were initially localized on a large s
patial scale within a single planetesimal which possibly suggests inco
rporation of preaccretionary objects as large as 0.1x of the final mas
s of the ordinary chondrite parent body.