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On the possibility of a second kind of mantle plume

机译:关于第二种地幔柱的可能性

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Results from recent tomographic imaging of the mantle have revealed plume-like structures under some hotspots and renewed the interest in the theoretically possible forms of ascending jets in mantle convection. It is now a classical view that plumes reaching the lithosphere from below can, in principle, develop from boundary layers either at 660 km or at 2900 km depth. If both types are present in the mantle, the 660 km boundary layer, possibly due to the endothermic spinel-perovskite phase transition, must be partially penetrable. The present study shows that, with a partially penetrable phase boundary at 660 km depth, a further kind of plumes can develop, namely from below the 660 km boundary layer. These 'mid-mantle plumes' have no root in the deep lower mantle. If, as recent viscosity inversions suggest, a second low viscosity zone exists under the 660 km discontinuity, then this 'second asthenosphere' represents a well-focused source volume for the mid-mantle plumes. These upwellings are the counterparts of avalanche-like downwellings crossing the phase boundary in an intermittent manner. The condition for the development of mid-mantle plumes is that the phase boundary acts as a strong, but not fully impenetrable barrier to vertical flow. In two- and three-dimensional numerical simulations using a compressible fluid in a Cartesian box, it has been found that the critical parameters of mantle convection (Rayleigh number, phase transition characteristics) closely meet this condition. Midmantle plumes develop with an eruptive vigor, much faster than the boundary layer plumes and can produce huge plume heads, exceeding 1000 km in radius. They can thus explain very extensive, episodic flood basalt volcanism on the surface. If mid-mantle plumes really exist, they can contribute to the explanation of the diversity of hotspot basalt isotopic signatures since they sample a geochemical reservoir distinct from the classical plume sources.
机译:最近对地幔进行层析成像的结果表明,在某些热点下呈羽状结构,并重新引起了人们对地幔对流中上升喷流的理论可能形式的兴趣。现在已成为经典观点,原则上可以从边界层以660 km或2900 km的深度形成从下方进入岩石圈的羽流。如果两种类型都存在于地幔中,则可能由于吸热的尖晶石-钙钛矿相变而在660 km边界层中部分渗透。本研究表明,在660 km深度处具有部分可穿透的相边界,可以从660 km边界层以下发展出另一类羽流。这些“中地幔柱”在深部下地幔中没有根源。如果像最近的粘度反演所暗示的那样,在660 km的不连续面下存在第二个低粘度带,那么这个“第二个软流圈”就代表着中地幔柱集中的源体积。这些上升流是雪崩状下降流以相交方式跨越相界的对应物。中地幔柱发育的条件是,相边界对垂直流起着很强但不能完全穿透的屏障的作用。在使用笛卡尔盒中的可压缩流体进行的二维和三维数值模拟中,已经发现地幔对流的关键参数(瑞利数,相变特性)非常满足此条件。中地幔柱具有爆发力,比边界层的羽层要快得多,并且可以产生巨大的羽根,半径超过1000 km。因此,他们可以解释表面上非常广泛的,偶发性的玄武岩洪水。如果确实存在中地幔柱,则它们可以对玄武岩热点同位素特征的多样性做出贡献,因为它们采样的地球化学储层不同于传统的羽源。

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