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Composite magnetic anisotropy fabrics: experiments, numerical models and implications for the quantification of rock fabrics

机译:复合磁各向异性织物:实验,数值模型和岩石织物量化的含义

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摘要

Magnetic fabrics from rocks with multiple mineral-preferred orientations may have anisotropy ellipsoids whose shape and orientation arise from the addition of two or more component fabrics. Our numerical models and experiments demonstrate that such composite magnetic fabrics do not directly reflect the shapes and/or orientations of the individual mineral fabrics and we provide criteria for the recognition and interpretation of composite fabrics in natural rocks. These criteria include: 1. (1) the orientation of the maximum susceptibility axis is located at the intersection of two planar fabrics, and2. (2) the shape of the susceptibility ellipsoid changes from oblate to prolate and the degree of anisotropy decreases, as the relative intensity of two planar component fabrics becomes equal and as the angle between the planar fabrics increases.Composite magnetic fabrics are observed in the shales and slates of the Martinsburg Formation, Lehigh Gap, Pennsylvania. Modeling of the AMS (anisotropy of magnetic susceptibility) and ARMA (anhysteretic remanent magnetization anisotropy) behavior constrains the relative degree of anisotropy of the bedding-parallel and cleavage-parallel fabrics. In particular, ARMA model results allow a good estimate of magnetite fabric strength.We conclude that, in the presence of composite magnetic fabrics, quantitative measures of finite strain in deformed rocks are limited by the ability to accurately determine the degree of anisotropy and relative susceptibility of each component fabric. Such determinations require knowledge of the mineral(s) that are responsible for the measured magnetic fabric and their behavior during deformation.
机译:具有多种矿物优先取向的岩石制成的磁性织物可能具有各向异性的椭球体,其形状和取向是由于添加了两种或多种组分织物而引起的。我们的数值模型和实验表明,这种复合磁性织物不能直接反映单个矿物织物的形状和/或方向,并且我们为识别和解释天然岩石中的复合织物提供了标准。这些标准包括:1.(1)最大磁化率轴的方向位于两个平面织物的相交处,以及2。 (2)当两种平面成分织物的相对强度相等且平面织物之间的夹角增加时,磁化率椭球的形状由扁长变为扁长且各向异性程度减小,在页岩中观察到复合磁性织物和宾夕法尼亚州里海峡的马丁斯堡组的板岩。 AMS(磁化率各向异性)和ARMA(磁滞剩余磁化各向异性)行为的模型约束了平行平行和平行平行织物的相对各向异性程度。特别是,ARMA模型的结果可以很好地估算磁铁矿织物的强度。我们得出结论,在存在复合磁性织物的情况下,变形岩石中有限应变的定量测量受到准确确定各向异性程度和相对磁化率的能力的限制。每个组成面料。此类确定需要了解负责测量的磁性织物的矿物及其在变形过程中的行为。

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