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Influence of melt on the creep behavior of olivine-basalt aggregates under hydrous conditions

机译:含水条件下熔体对橄榄石-玄武岩骨料蠕变行为的影响

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摘要

The influence of melt on the creep behavior of olivine-basalt aggregates under hydrous conditions has been investigated by performing a series of high-temperature triaxial compression experiments. Samples with melt fractions of 0.02 ≤ φ ≤ 0.12 were deformed under water-saturated conditions at temperatures between 1373 and 1473 K and a confining pressure of 300 MPa in a gas-medium apparatus. At constant differential stress and temperature, the rate of deformation increased rapidly but systematically with increasing melt fraction. In the diffusion creep regime, at a given differential stress, samples with melt fractions of 0.02 and 0.12 deformed a factor of ~2 and ~20, respectively, faster than a melt-free sample. In the dislocation creep regime, a sample with a melt fraction of 0.12 deformed a factor of ~40 faster than a melt-free sample. For partially molten olivine-basalt aggregates deformed under hydrous conditions, the dependence of creep rate on melt fraction can be expressed in the form ε(φ) = ε(0) exp(αφ), where α ≈ 26 for diffusion creep and α ≈ 31 for dislocation creep. The results of this study, combined with reasonable estimates for the spatial variation in the concentrations of water and melt (as well as for the geotherm and the activation volume for creep), provide constraints on the viscosity structure of Earth's upper mantle. As an example, we present a viscosity profile for the mantle wedge above a subducting plate, demonstrating that the viscosity in that region can vary by ~ 3 orders of magnitude over a depth of ~ 60 km due to the combined effects of water and melt weakening.
机译:通过进行一系列高温三轴压缩实验,研究了熔体对含水条件下橄榄石-玄武岩聚集体蠕变行为的影响。在气体介质装置中,将熔融分数为0.02≤φ≤0.12的样品在水饱和条件下于1373和1473 K之间的温度和300 MPa的限制压力下变形。在恒定的应力差和温度下,变形速率迅速增加,但随着熔体分数的增加而有系统地增加。在扩散蠕变状态下,在给定的不同应力下,熔体分数为0.02和0.12的样品的变形系数分别为无熔体的〜2和〜20倍。在位错蠕变状态下,熔体分数为0.12的样品比无熔体的样品变形快40倍。对于在含水条件下变形的部分熔融橄榄石-玄武岩聚集体,蠕变速率对熔体分数的依赖性可以表示为ε(φ)=ε(0)exp(αφ),其中对于扩散蠕变,α≈26,对于α≈ 31用于位错蠕变。这项研究的结果,加上对水和熔体浓度(以及地热和蠕变激活量)的空间变化的合理估计,为地球上地幔的黏度结构提供了限制。例如,我们给出了俯冲板上方地幔楔的粘度曲线,表明由于水和熔体弱化的共同作用,该区域的粘度在约60 km的深度上可以变化〜3个数量级。 。

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