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Buoyant melting instabilities beneath extending lithosphere: 2. Linear analysis

机译:延伸岩石圈以下的浮力融化不稳定性:2.线性分析

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In a companion paper, numerical models reveal that buoyant melting instabilities can occur beneath extending lithosphere for a sufficiently small mantle viscosity, extension rate, and rate of melt percolation. However, in some cases, instabilities do not develop during extension but only occur after extension slows or stops. These results are suggestive of a critical behavior in the onset of these kinds of instabilities and motivate a linear analysis to study the onset of instability in a partially melting, passively upwelling plane layer of mantle beneath extending lithosphere. The model we employ includes the effects of buoyancy arising from thermal expansion, the presence of a retained fraction of partial melt, and depletion of the solid by melt extraction. We find a critical behavior in the onset of instability controlled by melt retention buoyancy that is characterized by a “Rayleigh” number M, such that M must exceed some critical value M crit which depends on the efficiency of Stokes rise of a partially molten body relative to the rate of background percolation. Comparison of this theory to the numerical results in the companion paper yields a close quantitative agreement. We also find that solid depletion buoyancy can either stabilize or destabilize a partially melting layer, depending upon both the distribution of preexisting depletion and the magnitude of density changes with depth. This theory is compared with previous studies of buoyant melting instabilities beneath mid-ocean ridges where similar behavior was reported, and it suggests that the stability of passively upwelling, partially melting mantle underlying both narrow and wide rift settings is controlled by similar processes.
机译:在随附的论文中,数值模型表明,对于足够小的地幔粘度,扩展速率和熔体渗流速率,岩石扩展层下方可能会发生浮力融化不稳定性。但是,在某些情况下,不稳定性在扩展过程中不会发展,而只会在扩展变慢或停止后才发生。这些结果表明,在这类不稳定性的发生过程中存在关键行为,并激发了线性分析,以研究延伸的岩石圈下方部分熔融,被动上升的地幔平面层中的不稳定性的发生。我们采用的模型包括热膨胀产生的浮力,部分熔体保留部分的存在以及通过熔体萃取而使固体耗竭的影响。我们发现由熔体保持浮力控制的不稳定性开始时的临界行为,其特征是“瑞利”数M,使得M必须超过某个临界值M crit,该临界值取决于部分熔融体相对于斯托克斯上升的效率本底渗透率。将该理论与随附论文中的数值结果进行比较,得出了密切的定量一致性。我们还发现,固体耗尽浮力既可以稳定也可以使部分熔融层不稳定,这取决于既存耗尽的分布以及密度随深度变化的大小。将该理论与先前关于中海脊下方浮力融化不稳定性的研究进行了比较,该研究报告了类似的行为,它表明,在上下裂谷环境下被动上升的,部分融化的地幔的稳定性受类似过程控制。

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