Fractional melting and smelting on the ureilite parent body

被引:85
作者
Goodrich, Cyrena Anne
Van Orman, James A.
Wilson, Lionel
机构
[1] Kingsborough Community Coll, Dept Phys Sci, Brooklyn, NY 11235 USA
[2] Case Western Reserve Univ, Dept Geol Sci, Cleveland, OH 44106 USA
[3] Univ Lancaster, Dept Environm Sci, Inst Environm & Nat Sci, Lancaster LA1 4YQ, England
[4] Univ Hawaii Manoa, Sch Ocean & Earth Sci & Technol, Hawaii Inst Geophys & Planetol, Honolulu, HI 96822 USA
基金
美国国家科学基金会; 美国国家航空航天局;
关键词
D O I
10.1016/j.gca.2007.03.023
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
We investigate petrologic and physical aspects of melt extraction on the parent asteroid of the ureilite meteorites (UPB). We first develop a petrologic model for simultaneous melting and smelting (reduction of FeO by C) at various depths. For a model starting composition, determined from petrologic constraints to have been CV-like except for elevated Ca/Al (2.5 x CI), we determine (1) degree of melting, (2) the evolution of mg, (3) production Of CO + CO2 gas and (4) the evolution of mineralogy in the residue as a function of temperature and pressure. We then use these relationships to examine implications of fractional vs. batch melt extraction. In the shallowest source regions (similar to 30 bars), melting and smelting begin simultaneously at similar to 1050 degrees C, so that mg and the abundance of low-Ca pyroxene (initially pigeonite, ultimately pigeonite + orthopyroxene) begin to increase immediately. However, in the deepest source regions (similar to 100 bars), smelting does not begin until similar to 1200 degrees C, so that mg begins to increase and low-Ca pyroxene (pigeonite) appears only after similar to 21% melting. The final residues in these two cases, obtained just after the demise of augite, match the end-members of the ureilite mg range (similar to 94-76) in pyroxene abundance and type. In all source regions, production of CO + CO2 by smelting varies over the course of melting. The onset of smelting results in a burst of gas production and very high incremental gas/melt ratios (up to similar to 2.5 by mass); after a few % (s)melting, however, these values drastically decline (to < 0.05 in the final increments). Physical modelling based on these relationships indicates that melts would begin to migrate upwards after only similar to 1-2% melting, and thereafter would migrate continuously (fractionally) and rapidly (reaching the surface in < a year) in a network of veins/dikes. All melts produced during the smelting stage in each source region have gas contents sufficient to cause them to erupt explosively and be lost. However, since in all but the shallowest source regions part of the melting sequence occurs without smelting, fractional melting implies that a significant fraction of UPB melts may have erupted more placidly to form a thin crust (similar to 3.3 km thick for a 100 km radius body). Our calculations suggest that melt extraction was so rapid that equilibrium trace element partitioning may not have been attained. We present a model for disequilibrium fractional melting (in which REE partitioning is limited by diffusion) on the UPB, and demonstrate that it produces a good match to the ureilite data. The disequilibrium model may also apply to trace siderophile elements, and might help explain the "overabundance" of these elements in ureilites relative to predictions from the smelting model. Our results suggest that melt extraction on the UPB was a rapid, fractional process, which can explain the preservation of a primitive oxygen isotopic signature on the UPB. (c) 2007 Elsevier Ltd. All rights reserved.
引用
收藏
页码:2876 / 2895
页数:20
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