A Basin Model for Massive Banded Iron-Formations and its Geophysical Applications
A Basin Model for Massive Banded Iron-Formations and its Geophysical Applications
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块状带状铁矿盆地模型及其地球物理应用
DOI:
10.1086/628887
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发表时间:
1984
期刊:
影响因子:
--
通讯作者:
J. L. Cisne
中科院分区:
文献类型:
--
作者:
J. L. Cisne
Because banded iron-formation (BIF) density evidently decreased toward upper asthenosphere density with increasing water depth, feedback between sediment density and water depth by way of sedimentation-driven subsidence should have modulated the sediments' bulk density to the upper asthenosphere's. This mechanism helps explain why massive BIF's in longer wavelength, continental shelf basins have a more or less uniform bulk composition, and why their bulk densities closely correspond to the modern upper asthenosphere's. The difference between BIF and upper mantle densities in a short wavelength basin yields a rough estimate of the lithosphere's flexural rigidity. The elastic lithosphere of the Witwatersrand Basin, South Africa, 2.7 b.y. ago was about half as thick as typical modern continental lithosphere. Dynamic effects associated with isostatic equilibration yield estimates of the asthenosphere's dynamic viscosity to few hundred km depths. The fluid mantle beneath the Hamersley Basin, Australia, 2.5 b.y. ago was about as viscous as the modern low velocity zone. To the extent that accumulation and storage of iron in massive BIF's played a key role in lowering dissolved iron concentrations to required levels in the deep ocean, buildup of free oxygen there, if not in the atmosphere, must have had to await the growth of large continents with passive margins-for the lithosphere's flexural rigidity should effectively have limited thick BIF's to broad continental shelves.