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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 >Electrical conductivity of basaltic and carbonatite melt-bearing peridotites at high pressures: Implications for melt distribution and melt fraction in the upper mantle
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Electrical conductivity of basaltic and carbonatite melt-bearing peridotites at high pressures: Implications for melt distribution and melt fraction in the upper mantle

机译:高压下玄武岩和碳酸盐岩溶橄榄岩的电导率:对上地幔中熔体分布和熔体分数的影响

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Electrical impedance measurements were performed on two types of partial molten samples with basaltic and carbonatitic melts in a Kawai-type multi-anvil apparatus in order to investigate melt fraction-conductivity relationships and melt distribution of the partial molten mantle peridotite under high pressure. The silicate samples were composed of San Carlos olivine with various amounts of mid-ocean ridge basalt (MORB), and the carbonate samples were a mixture of San Carlos olivine with various amounts of carbonatite. High-pressure experiments on the silicate and carbonate systems were performed up to 1600K at 1.5GPa and up to at least 1650K at 3GPa, respectively. The sample conductivity increased with increasing melt fraction. Carbonatite-bearing samples show approximately one order of magnitude higher conductivity than basalt-bearing ones at the similar melt fraction. A linear relationship between log conductivity (σ_(bulk)) and log melt fraction (Φ) can be expressed well by the Archie's law (Archie, 1942) (σ_(bulk)/σ_(melt)=CΦ~n) with parameters C=0.68 and 0.97, n=0.87 and 1.13 for silicate and carbonate systems, respectively. Comparison of the electrical conductivity data with theoretical predictions for melt distribution indicates that the model assuming that the grain boundary is completely wetted by melt is the most preferable melt geometry. The gradual change of conductivity with melt fraction suggests no permeability jump due to melt percolation at a certain melt fraction. The melt fraction of the partial molten region in the upper mantle can be estimated to be 1-3% and ~0.3% for basaltic melt and carbonatite melt, respectively.
机译:为了研究高压下部分熔融地幔橄榄岩的熔融分数-电导率关系和熔融分布,在Kawai型多砧装置中对两种类型的具有玄武质和碳酸盐熔融物的部分熔融样品进行了电阻抗测量。硅酸盐样品是由圣卡洛斯橄榄石和各种数量的中洋脊玄武岩(MORB)组成的,碳酸盐样品是圣卡洛斯橄榄石和各种含量的碳酸盐的混合物。在硅酸盐和碳酸盐体系上进行的高压实验分别在1.5GPa下达到1600K和在3GPa上达到至少1650K。样品电导率随熔体分数的增加而增加。在相似的熔体分数下,含碳酸钙的样品的电导率比含玄武岩的样品高约一个数量级。对数电导率(σ_(体))和对数熔体分数(Φ)之间的线性关系可以通过阿奇定律(Archie,1942)(σ_(体)/σ_(熔体)=CΦ〜n)很好地表达硅酸盐和碳酸盐体系分别为= 0.68和0.97,n = 0.87和1.13。将电导率数据与熔体分布的理论预测进行比较表明,假设晶界被熔体完全润湿的模型是最优选的熔体几何形状。电导率随熔体分数的逐渐变化表明,由于在一定熔体分数下的熔体渗滤,导磁率没有跳跃。对于玄武质熔岩和碳酸盐熔岩,上地幔中部分熔融区域的熔体分数可以分别估计为1-3%和〜0.3%。

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