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1.
简要回顾了熔体形态学的研究方法，并分别从熔体分数和熔体分布形态两个方面，综合前人在熔体对岩石物理和力学性质的影响领域的主要研究成果，认为在部分熔融初期，熔体分数小，熔体主要分布于孤立的熔体囊内，对岩石的电学性质和力学性质影响不大，但是，对岩石的弹性波波速影响却很明显；随着熔体分数的增大，孤立的熔体囊逐渐连通形成熔体管道网络，岩石的电学性质发生显著变化；当熔体分数增至某一临界数值时，岩石体系结构改变，岩石的力学性质发生突变. 相似文献
2.
为了观测含碳酸盐地幔岩部分熔融过程中电导率的变化,厘清碳酸盐熔体在金伯利岩岩浆形成过程中所起的作用,并探讨Slave克拉通中部Lac de Gras地区约80～120km深处的高导成因,我们利用DS 3600t六面顶压机和Solartron 1260阻抗/增益-相位分析仪在1.0～3.0GPa、673～1873K温压条件下分别测量了含碳酸钠(Na_2CO_3)、碳酸钙(CaCO_3)和大洋中脊玄武岩(MORB)的地幔岩样品的电导率.实验结果表明,地幔岩样品的电导率主要受到温度和组分的影响,而压力对其影响较小.在温度低于1023K时,含Na_2CO_3地幔岩样品的电导率明显高于含同比重CaCO_3和MORB的;温度达到1023K时,含Na_2CO_3地幔岩样品开始熔融;但在之后的200K温度区间内,该部分熔融样品的电导率随温度的增加几乎不发生变化.这一现象或许揭示:地幔深部的碳酸质岩浆在快速上升过程中会同化吸收岩石圈地幔中的斜方辉石(Opx),进而形成金伯利岩岩浆,期间岩浆的电导率几乎不发生变化.含CaCO_3和MORB的地幔岩样品分别在1723K和1423K开始熔融,其部分熔融样品的电导率随温度的增加而快速增加.依据前人的研究结果和我们的实验结果,我们认为可以用含碳酸盐的部分熔融样品来解释Slave克拉通中部Lac de Gras地区约80～120km深处的异常高导现象,并推测熔体中碳酸盐的熔体比例小于2wt.%. 相似文献
3.
本文采用热弹性有限元数值模拟方法,计算二维情况下部分熔融花岗岩的纵波速度(Vp),分析熔体含量及熔体分布形态对于花岗岩纵波速度的影响.模拟结果表明花岗岩的Vp随着熔体含量的增加而降低,当熔体含量为7%～13%时,Vp可降至5.6～5.8km/s.熔体的形状对于Vp也有影响,当熔体以菱形形状分布于岩石中时,沿菱形长轴方向Vp减小幅度更大,在熔体含量达到15%时,沿菱形长轴方向的Vp减小达到20%,而在短轴方向仅4%.当熔体聚集成条带时,不同方向得到的Vp呈现明显的差异,表明熔体的定向排列不仅会使纵波速度呈现大幅度的减小,而且会引起地震波的各向异性. 相似文献
4.
以岩石实验中矿物的几何形态及空间分布为建模依据,以实验条件及单矿物电导率的测量结果为约束条件,用有限元数值方法模拟了不同微观结构的斜长石、辉石混合物在施加电压后电势及电流的分布情况,并计算了混合模型在不同温度条件下的电导率.研究结果显示,数值模型网格数及矿物颗粒数的选取对电导率计算结果的精度有较大影响,在体导电情况下,模型电导率因矿物比例含量和排列结构而异.当斜长石及辉石随机分布时,随着辉石含量的增加,混合模型电导率在不同温度下均有所增加,且温度越高,增加幅度越大,电导率的有限元模拟计算结果接近于有效介质渗透理论模型,且位于并、串联模型之间以及HS模型的上、下边界范围内;在斜长石及辉石含量一定的情况下,各矿物的排列分布对电导率计算结果也有一定的影响,当矿物颗粒大小接近且分布均匀时,模型中电势沿电流传导方向变化较为均匀,模拟计算得出的电导率相对较高,当矿物颗粒大小差别较大及分布不均匀时,电势分布受到一定的扰动,电导率计算结果也较低.将混合模型电导率有限元计算结果与辉长岩、辉绿岩及玄武岩实验测量结果进行比较,显示这3种岩石样品电导率与温度变化关系的斜率均与混合模型计算结果的斜率相接近,表明这些岩石在所选温度段导电机制与斜长石、辉石混合模型相似,用斜长石、辉石混合模型的电导率研究玄武岩、辉长岩及辉绿岩的导电性具有适用性.将混合模型有限元计算结果与玄武岩、辉长岩、辉绿岩覆盖区地壳大地电磁实测结果对比,发现大地电磁电导率结果位于混合模型计算结果范围内,用斜长石、辉石混合模型模拟玄武岩、辉长岩等岩石地壳具有一定的可行性. 相似文献
5.
深部岩石的弹性波各向异性是人们了解地壳深部构造特征,分析其成因,探讨其动力学意义的重要岩石物理参数。实验结果表明由矿物晶格定向分布(LPO)所引起的地壳岩石平均各向异性强度通常不超过5%,远不足以解释在青藏高原地壳中所观测到的弹性波各向异性之强度。模拟结果显示,熔体的定向分布(MPO)能够引起强烈的弹性波各向异性。例如,当熔体的形态因子(α)值介于0.1～0.5之间,熔融程度为5%～10%时,由定向分布的酸性熔体囊所产生的各向异性强度可以达到2%～10%(P波)、2.2～40%(S波)。众多研究资料显示,青藏高原—川滇西部具有加厚的中、上地壳和高地热梯度,低度部分熔融作用在其深部地壳中广泛存在。低度熔体在构造应力作用下的定向分布可能是造成该地区深部地壳存在异常强的各向异性层的重要原因。这暗示目前在青藏高原—川滇西部探测到的异常强的区域性各向异性层是具有部分熔融成因的强烈构造变形带。该构造变形带具有潜在的"解耦"功能,并作为地壳浅部刚性层(块体)的底界协调着块体与其下伏地壳或岩石圈地幔的差异运动。 相似文献
6.
7.
《中国科学:地球科学》2015,(9)
俯冲隧道模型提出,俯冲板片界面相互作用是实现地球表层与内部之间物质和能量交换的基本机制.由于大陆岩石圈与大洋岩石圈在物质组成和状态上的显著差异,其深部物理和化学过程及壳幔相互作用产物必然出现一系列差异.许多实验岩石学研究已经为大洋俯冲隧道中可能发生的硅酸盐和碳酸盐岩石的部分熔融和壳幔相互作用提供了资料.无论是基性还是中酸性硅酸盐岩体系,取决于部分熔融发生的压力或深度,熔体是具有或不具有埃达克岩性质的花岗质熔体.微量CO2即可大幅降低橄榄岩的熔点,所形成的碳酸盐熔体可有效萃取岩石体系中不相容微量元素.这些硅饱和或不饱和熔体均可以在俯冲隧道或地幔深部条件下与地幔楔橄榄岩发生反应,形成复杂的反应过程和产物.但已有的实验结果主要是针对大洋岛弧环境条件而不是大陆俯冲带的环境.因此,高温高压实验需要充分考虑大陆俯冲隧道中板片-地幔界面上各种不同成分地壳及其衍生的熔/流体成分与不同橄榄岩之间的反应,并结合大陆俯冲带岩石部分熔融和壳幔相互作用的地质证据,以阐明大陆俯冲隧道过程中的变质脱水、部分熔融和地幔交代等问题. 相似文献
8.
建立了南北地震带北段下地壳部分熔融几何形状和分布的模型。熔融的几何分布和连通性由以下3个因素决定：①熔融的位置;②熔融所占总体积的比例;③固－固和固－液界面的最小自由能。熔融形状有薄版形、管道形和椭球包体形。用此模型计算出含有部分溶融岩石的体积、剪切弹性模量和电导率的一般表示式。选择参数并计算出南北地震带北段下地壳的Vp、Vs和电阻率ρs值,即在鄂尔多斯地台下地壳的速度为Vp ≈6.71km/s,Vs≈3.96km/s,电阻率为上百至几百欧姆米。而在祁连、秦岭褶皱系下地壳速率Vp约为6．4～6.6km/s,Vs约为3．72～3．89km/s,电阻率为几至几十欧姆米。数值模拟的结果与地球物理反演结果基本相符,并进行了定性的构造解释。用一个模型对下地壳中的速度特征与电性特性进行了联合数值模拟,说明了此模型在解释下地壳中的Vp、Vs和ρs的有效性。 相似文献
9.
地幔过渡带顶部低速层的成因及性质研究,对于认识地球内部物质运移及地幔对流过程等具有非常重要的动力学意义.最新的地震学研究显示,华南陆块东部地幔过渡带顶部的低速层存在着明显的区域性差异.一般认为,该低速层的形成与脱水引起的部分熔融有关.本文利用部分熔融体系的平衡几何模型,重点分析了熔体成分、位温、二面角和玄武质含量等因素对熔体含量的影响,并结合该低速层的分布特征,估算出研究区的南北两个子区域地幔过渡顶部熔体含量分别为~1.18vol.%和~2.02vol.%.这一熔体含量的显著差异可能与太平洋板片多期次俯冲作用的叠加有关. 相似文献
10.
《中国科学:地球科学》2016,(4)
大地电磁测深与电导率测量相结合已经成为探索地球内部状态的有效手段.含水硅酸盐熔体和富水流体的电导率显著高于硅酸盐矿物,而且对成分和温压条件十分敏感,可以用于认识深部的部分熔融和流体活动.本文系统总结了含水硅酸盐熔体和富水流体电导率的实验研究现状,并介绍了相关研究结果的若干重要应用.硅酸盐熔体电导率随温度上升而增大,随压强升高而减小.在Na~+含量相当的前提下,钙碱性系列熔体电导率从玄武质到流纹质呈上升趋势,其活化焓呈下降趋势.水的加入令熔体电导率显著增大,其主要原因在于增强了阳离子的活动性.流体电导率研究主要集中在稀电解质溶液.溶液电导率随温度上升先增大后减小,随压强升高一般先增大,超过一定压强后基本保持不变.从电导率数据可以得到电解质的电离常数.为建立广泛适用的熔/流体电导率随温度、压强和成分变化的定量模型,还需要在实验方法创新的基础上,对更多具有代表性的体系开展大范围温压条件下的电导率实验研究. 相似文献
11.
Volker Haak 《Surveys in Geophysics》1980,4(1-2):57-69
Laboratory data of the electrical conductivity of rocks and minerals pertinent to the deeper crust and upper mantle and summarized. They are discussed in the context of a theory to calculate effective conductivities of materials in the state of partial melt. Most published data have been obtained by too rapid measurements, i.e. without reaching an equilibrium state of the sample. Conductivity measurements on a material similar to the composition of pyrolite are not het known, their importance is outlined. A global conductivity distribution obtained by electromagnetic induction studies is represented by a few results covering oceanic and continental areas. Till today it seems to be a doubtful venture to deduce the temperature of the upper mantle or even the existence of a partial molten asthenosphere from a global conductivity distribution. On a more local scale the correlation of electrical conductivity with temperature and state of the material seems to be more realistic. This is tentatively shown by two petrological models of the Afar depression in Ethiopia and of the midoceanic rift. 相似文献
12.
Electrical conductivity σ of two ultramafic rocks (a spinel lherzolite and a garnet peridotite) has been investigated to melting temperature at 1 bar under known oxygen fugacity environment. The electrical conductivity of the two rocks is found to increase with degree of partial melting and an ～ 15% melt fraction is necessary for the electrical conductivity to increase by ～ 1 order of magnitude. For a given melt fraction electrical conductivity of a spinel lherzolite is lower than that of a garnet peridotite and may be attributed to the differences in the composition of the melts formed. 相似文献
13.
The resistance to current flow of minerals and partial-melts is a frequency dependent electrical property. Measurements of the frequency dependent electrical impedance of single crystal olivine, polycrystalline olivine, dunites, metapelites, and partial-melts, between 10–4 and 105 Hz, when plotted in the complex impedance plane, reveal arcs that correspond to different conduction mechanisms in the material being studied. In polycrystalline materials, two impedance arcs related to material properties (as opposed to electrode properties or electrode-sample interactions) are observed. Each impedance arc is activated over a distinct range of frequency, that is, the mechanisms occur in series. Based on experiments comparing single and polycrystalline impedance spectra, experiments on samples with different electrode configurations, and on samples of varying dimension, the mechanisms responsible for these impedance arcs are interpreted as grain interior conduction (
gi
), grain boundary conduction (in polycrystalline materials;
gb
), and sample-electrode interface effects, from highest to lowest frequency, respectively. Impedance spectra of natural dunitic rocks reveal analogous behavior, that is,
gb
and
gi
add in series. The grain boundaries do not enhance the conductivity of any of the materials studied (a direct result of the observed series electrical behavior) and, under certain conditions, limit the total conductivity of the grain interior-grain boundary system. By examining the frequency dependence of the electrical properties of partial-melts, it is possible to gain information about microstructure and the distribution of the melt phase and to determine the conditions under which the presence of melt enhances the total conductivity. Impedance spectra of olivine-basalt partial-melts indicate that at least two conduction mechanisms occur in series over the frequency range 10–4-105 Hz, similar to the observed electrical response of melt-absent polycrystalline materials. In a sample containing isolated melt pockets the intermediate frequency grain boundary impedance arc is modified by the presence of melt indicating series conduction behavior. In a sample with an interconnected melt phase the high frequency grain interior impedance arc is modified by the melt phase, indicating the initiation of parallel conduction behavior. Because field EM response versus frequency curves are used to derive conductivity versus depth profiles, it is important to perform laboratory experiments to understand the frequency-dependent electrical behavior of Earth materials. Activation energies determined from studies that measure conductivity at a single frequency may be erroneous because of the shift of the dominant conduction mechanism with frequency as temperature is varied. 相似文献
14.
Interrelations Between Thermal Conductivity and Other Physical Properties of Rocks: Experimental Data 总被引：2，自引：0，他引：2
Y. Popov V. Tertychnyi R. Romushkevich D. Korobkov J. Pohl 《Pure and Applied Geophysics》2003,160(5-6):1137-1161
— A new non-contact and non-destructive optical scanning instrument provided a large number of high-precision measurements of thermal conductivity tensor components in samples of sedimentary and impact rocks, as well as new insights into interrelations between thermal conductivity and other physical properties. More than 800 core samples (dry and fluid-saturated) of sedimentary rocks from different Russian oil-gas deposits and impact rocks from the well “Nördlingen 1973” drilled in the Ries impact structure (Germany) were studied using optical scanning technology. It was established that the thermal conductivity parallel to the stratification is more informative for petrophysical investigations than the thermal conductivity perpendicular to the layering. Different approaches were developed to estimate porosity, permeability, pore space geometry, and matrix thermal conductivity with a combination of thermal conductivity measurements in dry and fluid-saturated samples and mathematical modelling. These approaches allow prediction of the rock porosity and permeability and their spatial distribution along a well using thermal conductivity measurements performed with the optical scanning instrument directly applied to cores. Conditions and constraints for using Lichtenecker-Asaad's theoretical model for the estimation of porosity and thermal conductivity of sedimentary rocks were determined. A correlation between thermal conductivity and acoustic velocity, porosity, density, and electric resistivity of impact rocks was found for different rock types. New relationships between permeability, electrical and thermal conductivity found for sedimentary rocks are described. 相似文献
15.
Harve S. Waff 《Surveys in Geophysics》1980,4(1-2):31-41
This paper examines the constraint placed by electrical conductivity on physical conditions existing within the mantle. Determination of bulk electrical conductivities of multiphase materials from knowledge of individual phase conductivities and their relative fractions is discussed in the light of recent studies of the equilibrium phase geometries of partial melts. It is concluded that existing models which are based on assumed geometries offer little refinement over Hashin-Shtrikman variational bounds. The possible effects of the gravitational field on phase geometry in partial melts and the resulting conductivity anisotropy are considered. At this time it appears that minimum melt fractions can be safely estimated from a knowledge of Earth conductivity combined with laboratory data on melt and crystalline conductivities and the Hashin-Shtrikman upper bound. The question of whether or not the asthenosphere corresponds to a zone of partial melting is also addressed. 相似文献
16.
碳是影响岩石电导率大小的一个重要因素,可能是造成龙门山断层带电导率异常的重要原因之一.为了研究不同的碳含量、矿物颗粒粒径与碳晶体结构对断层带电导率的影响,在干燥、常温、0.2~300 MPa的压力条件下实验研究了人工模拟断层泥样品(石英粉末与含碳粉末混合的样品,简称模拟样品)和采自映秀-北川断层八角庙剖面的天然断层岩样品(简称天然样品)的电导率.实验结果显示,当模拟样品中的含碳粉末连通时,电导率与碳体积率的关系符合逾渗理论模型;而含碳粉末未连通时,电导率随总孔隙度降低而指数性升高.同时模拟样品的电导率也随石英颗粒粒径的变化而发生改变.相比于模拟样品中的含碳粉末主要分布于石英颗粒支撑的孔隙中,天然样品中的碳则主要以碳膜的形式赋存在颗粒边缘,导致碳体积率相同的条件下,模拟样品的电导率小于天然样品.此外,天然样品的电导率(9×10~(-4)S·m~(-1))也要小于野外大地电磁探测的结果(0.03~0.1 S·m~(-1)).在今后的实验中还需要考虑在动态摩擦条件下对含有完整含碳结构的天然样品进行电导率的实验研究. 相似文献
17.
M. P. Ryan 《Bulletin of Volcanology》1980,43(4):743-772
A study of the elasticity of the solidus of igneous rocks provides a means of evaluating several high temperature mechanical characteristics of the zone that forms the transition region between solid rock and rock with a small fraction of partial melt — that is, the magma reservoirenvelope. This type of study has been performed for Hawaiian olivine tholeiite, by employing the theoretical treatment ofWalsh (1969). The effective aggregate bulk modulus (K*), aggregate rigidity (μ*), aggregate Young’s modulus (E*) and the aggregate Poisson’s ratio (n*) have been used to characterize the range in elastic behavior expected for this partially molten envelope. The details of mineralogy, mineral crystal chemistry and microstructure for a tholeiitic basalt from a deep-ponded flow unit (the Boiling Pots), as well as the geometry of melt pocket aspect ratios have been used to provide a basis for computing the elasticity for a shallow reservoir solidus. For a broad range in modal mineralogy, the internal 0–1% melt represents a transition region from an aggregate elasticity controlled by mineral composition, to an elastic behavior dominated by the melt phase (evaluated at a melt pocket aspect ratio ofε=0.001). For vesicular rocks in a low pressure environment, the internal 0–1% melt represents a transition from porosity-controlled elasticity to melt-controlled elasticity, evaluated at a prevalent aspect ratio ofε=0.001, and over the porosity range Φ=0.0?0.20 (20%). Thin melt films found to separate plagioclase microlites (0.0001=ε) are capable of effecting a 94.7% reduction in Young’s modulus, E*, over the 0–1% melt range, and suggest that the reservoir envelope may be critically weakened by rather small volume fractions of liquid, if dispersed in such narrow packets. 相似文献
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电导率是表征岩石电学性质的重要物理参数,在地质资源勘查和测井解释等领域发挥着巨大作用.快速、准确地确定岩石电导率具有重要的理论和实践意义.作为近年来发展的一种岩石物理数值模拟工具,数字岩心技术在定量计算电导率等物性参数方面应用广泛.三维微观结构的准确获取是数字岩心技术计算岩石电导率的关键,但传统获取岩石三维微观结构的方法较为复杂费时.为了方便快速地通过数字岩心技术计算岩石的电导率,本文研究了岩石二维与三维数字岩心的电导率联系.我们基于微米级X射线CT扫描得到的三个砂岩样品的微观结构信息建立了三维数字岩心,并通过有限元法计算的三维数字岩心电导率与实验数据的对比验证数值计算方法的有效性.随后我们数字地扩展了岩石的孔隙,产生了较大孔隙度的三维数字岩心样本,在此基础上,计算了三维数字岩心和相应二维数字岩心的电导率,并通过Archie公式分别拟合了电导率与孔隙度之间的关系,得到了相应的胶结系数.结果表明,三维数字岩心的胶结系数小于二维数字岩心的胶结系数,且二者的比值与岩石实测孔隙度呈线性负相关关系.以该联系为纽带,通过二维图像快速计算得到的电导率与孔隙度关系,确定了三维数字岩心的电导率与孔隙度关系,并进一步通过三维数字岩心的孔隙度计算其电导率.该方法计算得到的人工砂岩样品的电导率与其三维数字岩心电导率相关系数高于96%,验证了基于二维图像的数字岩心电导率计算方法的有效性.本文的研究结果为快速、准确地计算岩石电导率提供了新的思路,在油气勘探开发中有广阔的应用前景. 相似文献