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首页> 外文期刊>Earth and Planetary Science Letters: A Letter Journal Devoted to the Development in Time of the Earth and Planetary System >Estimates of olivine-basaltic melt electrical conductivity using a digital rock physics approach
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Estimates of olivine-basaltic melt electrical conductivity using a digital rock physics approach

机译:使用数字岩石物理学方法估算橄榄石-玄武岩熔体的电导率

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Estimates of melt content beneath fast-spreading mid-ocean ridges inferred from magnetotelluric tomography (MT) vary between 0.01 and 0.10. Much of this variation may stem from a lack of understanding of how the grain-scale melt geometry influences the bulk electrical conductivity of a partially molten rock, especially at low melt fraction. We compute bulk electrical conductivity of olivine-basalt aggregates over 0.02 to 0.20 melt fraction by simulating electric current in experimentally obtained partially molten geometries. Olivine-basalt aggregates were synthesized by hot-pressing San Carlos olivine and high-alumina basalt in a solid-medium piston-cylinder apparatus. Run conditions for experimental charges were 1.5 GPa and 1350 degrees C. Upon completion, charges were quenched and cored. Samples were imaged using synchrotron X-ray micro-computed tomography (mu-CT). The resulting high-resolution, 3-dimensional (3-D) image of the melt distribution constitutes a digital rock sample, on which numerical simulations were conducted to estimate material properties. To compute bulk electrical conductivity, we simulated a direct current measurement by solving the current continuity equation, assuming electrical conductivities for olivine and melt. An application of Ohm's Law yields the bulk electrical conductivity of the partially molten region. The bulk electrical conductivity values for nominally dry materials follow a power-law relationship sigma(bulk) = C sigma(melt)phi(m) with fit parameters m = 1.3 +/- 0.3 and C = 0.66 +/- 0.06. Laminar fluid flow simulations were conducted on the same partially molten geometries to obtain permeability, and the respective pathways for electrical current and fluid flow over the same melt geometry were compared. Our results indicate that the pathways for flow fluid are different from those for electric current. Electrical tortuosity is lower than fluid flow tortuosity. The simulation results are compared to existing experimental data, and the potential influence of volatiles and melt films on electrical conductivity of partially molten rocks is discussed. (C) 2015 Elsevier B.V. All rights reserved.
机译:根据大地电磁层析成像(MT)推断,快速扩散的中洋海脊下方的熔体含量估计值在0.01至0.10之间变化。这种变化的很大一部分可能是由于缺乏对晶粒尺度熔体几何形状如何影响部分熔融岩石的整体电导率的了解,尤其是在熔体分数低的情况下。我们通过模拟以实验方式获得的部分熔融几何形状中的电流,计算出熔体分数在0.02至0.20之间的橄榄石-玄武岩聚集体的整体电导率。橄榄石-玄武岩聚集体是通过在固态活塞缸设备中热压San Carlos橄榄石和高铝玄武岩合成的。实验装料的运行条件为1.5 GPa和1350摄氏度。完成后,将装料淬火并取芯。使用同步加速器X射线微计算机断层扫描(mu-CT)对样品进行成像。所得的熔体分布的高分辨率3维(3-D)图像构成了一个数字岩石样本,在其上进行了数值模拟以估计材料特性。为了计算体积电导率,我们通过求解电流连续性方程来模拟直流电测量,并假设橄榄石和熔体的电导率。欧姆定律的应用产生了部分熔融区域的整体电导率。标称干燥材料的总电导率值遵循幂律关系sigma(bulk)= C sigma(melt)phi(m),拟合参数m = 1.3 +/- 0.3和C = 0.66 +/- 0.06。在相同的部分熔融几何形状上进行了层流仿真,以获得渗透率,并比较了在相同熔融几何形状上的电流和流体流动的各自路径。我们的结果表明,流动流体的路径不同于电流的路径。电气弯曲度低于流体流动弯曲度。将模拟结果与现有实验数据进行了比较,并讨论了挥发物和熔膜对部分熔融岩石电导率的潜在影响。 (C)2015 Elsevier B.V.保留所有权利。

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