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首页> 外文期刊>Icarus: International Journal of Solar System Studies >Mantle dynamics in super-Earths: Post-perovskite rheology and self-regulation of viscosity
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Mantle dynamics in super-Earths: Post-perovskite rheology and self-regulation of viscosity

机译:超级地球的地幔动力学:钙钛矿后的流变学和粘度的自我调节

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摘要

The discovery of extra-solar "super-Earth" planets with sizes up to twice that of Earth has prompted interest in their possible lithosphere and mantle dynamics and evolution. Simple scalings suggest that super-Earths are more likely than an equivalent Earth-sized planet to be undergoing plate tectonics. Generally, viscosity and thermal conductivity increase with pressure while thermal expansivity decreases, resulting in lower convective vigour in the deep mantle, which, if extralopated to the largest super-Earths might, according to conventional thinking, result in no convection in their deep mantles due to the very low effective Rayleigh number. Here we evaluate this. First, as the mantle of a super-Earth is made mostly of post-perovskite we here extend the density functional theory (DFT) calculations of post-perovskite activation enthalpy of to a pressure of 1TPa, for both slowest diffusion (upper-bound rheology) and fastest diffusion (lower-bound rheology) directions. Along a 1600K adiabat the upper-bound rheology would lead to a post-perovskite layer of a very high (~10~(30)Pas) but relatively uniform viscosity, whereas the lower-bound rheology leads to a post-perovskite viscosity increase of ~7 orders of magnitude with depth; in both cases the deep mantle viscosity would be too high for convection. Second, we use these DFT-calculated values in statistically steady-state numerical simulations of mantle convection and lithosphere dynamics of planets with up to ten Earth masses. The models assume a compressible mantle including depth-dependence of material properties and plastic yielding induced plate-like lithospheric behaviour. Results confirm the likelihood of plate tectonics for planets with Earth-like surface conditions (temperature and water) and show a self-regulation of deep mantle temperature. The deep mantle is not adiabatic; instead feedback between internal heating, temperature and viscosity regulates the temperature such that the viscosity has the value needed to facilitate convective loss of the radiogenic heat, which results in a very hot perovskite layer for the upper-bound rheology, a super-adiabatic perovskite layer for the lower-bound rheology, and an azimuthally-averaged viscosity of no more than 10~(26)Pas. Convection in large super-Earths is characterised by large upwellings (even with zero basal heating) and small, time-dependent downwellings, which for large super-Earths merge into broad downwellings. In the context of planetary evolution, if, as is likely, a super-Earth was extremely hot/molten after its formation, it is thus likely that even after billions of years its deep interior is still extremely hot and possibly substantially molten with a "super basal magma ocean" - a larger version of the proposal of Labrosse et al. (Labrosse, S., Hernlund, J.W., Coltice, N. [2007]. Nature 450, 866-869), although this depends on presently unknown melt-solid density contrast and solidus.
机译:太阳超级“超地球”行星的发现是地球的两倍,这引起了人们对它们可能的岩石圈,地幔动力学和演化的兴趣。简单的缩放表明超级地球比同等大小的地球更有可能经历板块构造。通常,粘度和导热系数随压力的增加而热膨胀系数的降低,导致深地幔的对流活力降低,按照传统的思想,如果将其扩展到最大的超地球,可能会导致深地幔不对流到非常低的有效瑞利数。在这里,我们对此进行评估。首先,由于超级地球的地幔主要由钙钛矿后期构成,因此我们将钙钛矿后期活化焓为1TPa的密度泛函理论(DFT)计算扩展为最慢的扩散(上限流变学) )和最快的扩散(低边界流变学)方向。沿着1600K的绝热材料,上限流变会导致钙钛矿后层具有很高的(〜10〜(30)Pas)但相对均匀的粘度,而下限流变会导致钙钛矿后的粘度增加深度约为7个数量级;在这两种情况下,深地幔粘度对于对流都将太高。其次,我们将这些DFT计算的值用于具有最多10个地球质量的行星的地幔对流和岩石圈动力学的统计稳态数值模拟中。这些模型假定可压缩地幔包括材料属性的深度相关性和塑性屈服引起的板状岩石圈行为。结果证实了具有类似地球表面条件(温度和水)的行星的板块构造的可能性,并显示出深地幔温度的自我调节。深层地幔不是绝热的。取而代之的是内部加热,温度和粘度之间的反馈会调节温度,以使粘度具有促进对流辐射热损失所需的值,从而导致上部流变性的钙钛矿层非常热,即超级绝热钙钛矿层较低的流变学特性,方位平均粘度不超过10〜(26)Pas。大型超级地球的对流特征是大型上升流(即使基础加热为零)和小型的,与时间有关的下降流,对于大型超级地球而言,对流合并为宽泛的下降流。在行星演化的背景下,如果超级地球在形成后很可能非常热/融化,那么很可能即使在数十亿年之后,其深部内部仍然仍然非常热并且可能实质上融化了“超级基底岩浆海洋”-Labrosse等人的提议的较大版本。 (Labrosse,S.,Hernlund,J.W.,Coltice,N. [2007]。Nature 450,866-869),尽管这取决于目前未知的熔体-固相密度对比和固相线。

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