下地幔热通量大幅变化诱发的内核异质性

Aditya Varma, Binod Sreenivasan
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摘要

内核顶部的地震绘图显示出两个不同的高P波速度区域,一个位于亚洲下方,另一个位于大西洋下方。这种双重模式支持了下地幔异质性可以通过外核对流传递到内核的观点。在这项研究中,双成分对流动力模型(热对流接近临界,成分对流为强超临界)在快速旋转的地核强驱动机制中产生了大量的内核异质性。虽然模拟世俗冷却的温度曲线确保地幔异质性最远传播到内核边界(ICB),但内核边界的热通量分布是由成分浮力的强度决定的。地核-地幔边界(CMB)的热通量差$q^*$为$O(10)$,其中$q^*$为地核-地幔边界的最大热通量差与平均热通量之比。在这里,根据动力学中的 ICB 热通量估算出的 P 波速度在东部高于西部,半球差异与观测到的下限(0.5%)相同。在这一机制中,其他观测约束条件也得到了满足--东部高纬度磁通量的可变性低于西部;外核底部的分层F层由内核区域熔化产生的质量通量提供,并受到磁阻尼,其稳态高度为$\sim$ 200千米。
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Inner core heterogeneity induced by a large variation in lower mantle heat flux
Seismic mapping of the top of the inner core indicates two distinct areas of high P-wave velocity, the stronger one located beneath Asia, and the other located beneath the Atlantic. This two-fold pattern supports the idea that a lower-mantle heterogeneity can be transmitted to the inner core through outer core convection. In this study, a two-component convective dynamo model, where thermal convection is near critical and compositional convection is strongly supercritical, produces a substantial inner core heterogeneity in the rapidly rotating strongly driven regime of Earth's core. While the temperature profile that models secular cooling ensures that the mantle heterogeneity propagates as far as the inner core boundary (ICB), the distribution of heat flux at the ICB is determined by the strength of compositional buoyancy. A large heat flux variation $q^*$ of $O(10)$ at the core-mantle boundary (CMB), where $q^*$ is the ratio of the maximum heat flux difference to the mean heat flux at the CMB, produces a core flow regime of long-lived convection in the east and time-varying convection in the west. Here, the P-wave velocity estimated from the ICB heat flux in the dynamo is higher in the east than in the west, with the hemispherical difference of the same order as the observed lower bound, 0.5%. Additional observational constraints are satisfied in this regime -- the variability of high-latitude magnetic flux in the east is lower than that in the west; and the stratified F-layer at the base of the outer core, which is fed by the mass flux from regional melting of the inner core and magnetically damped, attains a steady-state height of $\sim$ 200 km.
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