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云南大硐厂铅锌矿床中的硫碲铋矿A 总被引:1,自引:0,他引:1
硫碲铋矿A产于云南省大硐厂铅锌矿床,与自然铋、辉铋铅矿共生。晶体呈柱状,粒度0.02 ̄0.3mm。反光显微镜下呈淡黄色,弱非均质性,反射率Rc′=52.4%,R0=48.8%(波长为540nm),显微压入硬度Hv=46 ̄72kg/mm^2。主要粉晶谱线:3.065(10),2.120(7),1.346(5),2.220(4)。三方晶系,空间群为D3d^5-R3↑-m,晶胞参数a=0.4241nm, 相似文献
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新矿物双峰矿—铱的二碲化物 总被引:2,自引:1,他引:2
双峰矿产在纯橄榄岩体铬矿体中。在铬矿石及矿体邻近的砂矿中均可找到,呈块状聚集体或板片状与硫铱矿、锇自然铱矿紧密共生。直径0.5 ̄0.2mm,脉状的宽0.05 ̄0.10mm,长0.5 ̄1.0mm。金属光泽。条痕黑色。H(M)3。VHN20108kg/mm^2(平均)。解理:(0001)完全。性脆。计算密度为10.14g/cm^3。反射色:亮黄白带蓝色调。内反射无。非均质性中等,偏光色为淡蓝或淡黄。双 相似文献
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共同-疙瘩沟地区金-多金属矿床(点)多产于燕山早期花岗岩中,矿体石英中流体包裹体较发育,以气液包裹体为主,通过流体包裹体的研究认为:成矿流体属于Na^+-Ca^2+-Cl^--(SO4)^2-型中,中一低盐度(5.7%~8.5%),成矿温度为中(偏低)温(225~275℃),压力为75.1~115.8MPa,pH为5.23~6.05,Eh为-0.57~-0.62V,推断Au最可能的搬运形式为(Au 相似文献
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冀东高级变质岩石的流体包裹体研究 总被引:5,自引:5,他引:5
冀东高级变质的石榴石斜长片麻岩、含或不含石榴石的角闪二辉斜长片麻岩、紫苏花岗岩、斜长角门岩等岩石中的流体包裹体主要有4类,按形成的先后顺序依次为:(1)H2O和CO2两液相包裹体,CO2的部分均一温度是-12℃,密度1.04g/cm3,H2O含量21%~39%(mole%),CO2含量50%~71%(mole%);(2)CO2液相包裹体,冰点温度-56℃~-61℃,均一温度-7.4℃~-35.1℃,CO2密度约为1.05g/cm3,CO2含量82.1%~98.4%(mole%),还有少量的CH4、N2和H2等组分;(3)H2O和CO2多相包裹体,CO2的部分均一温度7℃~28℃,CO2密度为0.64~0.93g/cm3,气相组分以CO2、CH4和CO为主,液相成分主要是H2O和CO2;(4)多世代盐水溶液包裹体,冰点温度-0.5℃~-20℃,盐度0.87%~22.8%(wt%),盐水密度0.7~1.05g/cm3,均一温度在150℃~200℃和约300℃,存在两个峰值。不同世代的流体包裹体记录了等密度降温的P-T路径。包裹体反映的变质作用早期降温过程流体的H2O/H2O+CO2(mole)比值降低,晚期升高 相似文献
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硅铁灰石是一种罕见的单链硅酸盐矿物,产于矿体围岩的晚期热液脉中,其晶体呈厚板状或矛头状,颗粒大小0.1mm—0.5mm,日光下呈黑色,强光源下呈浓茶绿色─棕色,玻璃光泽,条痕淡灰绿色,透明─半透明,维克显微硬度Hv100g=359kg·mm-2,实测密度3.35g·cm-3,计算密度为3.32g·cm-3。偏光显微镜下显正高突起,具强多色性,Ng浅黄棕色、Np暗绿色,二轴晶正光性,ZV(+)=76(1)°,折射率Ng=1.759,Nm=1.737,Np=1.728.X射线单晶衍射表明,硅铁灰石属三斜晶系,空间群为P1。由X射线粉晶衍射数据计算出晶胞参数a=0.7475(1)nm,b=1.1844(1)nm,c=0.6679(1)nm,α=91°34(3)′,β=93°45(1)′,γ=103°19(1)′。硅铁灰石的晶体化学式为(Ca2.071Na0.007K0.001)2.079(FeMnM0.171)0.991(FeAlTi0.002)1.021[(Si4.989 Al0.011)5.000O14.101(OH)0.899]。硅铁灰石是酸式硅酸盐,不存在与阳离子结合的OH-离子,因而在红外光谱中缺失34 相似文献
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河南鲁山早前寒武纪太华群中分布着两类斜长角闪岩:一类为正常斜长角闪岩,主要产于晚太古代下太华群荡泽河组;另一类为富钠斜长角闪岩,产于古元古代上太华群雪花沟组,两类岩石外表特征和矿物成分相近似,但化学成分明显不同,正常斜长角闪岩具较低的Na2O(1.96%-2.86%),K2O(0.24%-0.64%),Ti,Y,Zr,Hf和∑REE含量,而富钠的斜长角闪岩以较高的Na2O(3.31%-5.50%) 相似文献
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重点研究了414矿床石英流体包裹体特征及成矿物理化学条件,其成矿温度490~530℃;成矿压力为1080×10 ̄5Pa;成矿溶液的pH值为4.82~4.83;Eh值为-0.425~-0.436伏特,fo_2:为10 ̄(-30.44)~1O ̄(-30.09)。 相似文献
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考虑核电厂地基-基础的动力相互作用,应用显式动力有限差分法分析了地震作用下极软岩、较软岩、坚硬岩上核电厂建筑结构基础的地震响应特征,比较了岩石坚硬程度对基础加速度反应谱的影响。研究表明:随着岩石坚硬程度的提高,核电厂建筑物结构基础的地震响应有增加的趋势;在周期轴上,基础处的加速度反应谱曲线会随着岩石坚硬程度的提高逐渐向短周期(高频段)方向移动。在高频段,建造于较坚硬岩石上基础结构的加速度反应谱值偏大;在中等频段,建造于较软岩石上基础结构的加速度反应谱值偏大;在低频段,岩石坚硬程度对加速度反应谱的影响不显著。 相似文献
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M. D. Sharma 《Journal of Earth System Science》2004,113(2):247-257
Three dimensional scattering of near-field is studied for dilatation and rotation in the time domain. The perturbation method
is applied to solve the equation of motion for the first order scattering from a weak inhomogeneity in an otherwise homogeneous
medium. The inhomogeneity is assumed close enough to the point source so that the near-field intermediate wave is dominating
over the far-field sphericalP andS pulses. The integral expressions are derived to relate dilatation and rotation of scattering to the radial fluctuations of
velocities and density in the inhomogeneity. These integrals are solved to calculate the strains of scattering from (a part
of) an inhomogeneous spherical shell of arbitrary curvature. Variable curvature may allow the shape of inhomogeneity volume
element to change uniformly from spherical to rectangular. Rotation of scattering from a spherical shell is independent ofP wave velocity inhomogeneity. Dilatation of scattering does not involveS wave velocity inhomogeneity but its gradient. The back scattering results are obtained as a special case. Strains are computed
numerically, for hypothetical models to study the effects of various parameters viz., velocity inhomogeneity, distance of
source from inhomogeneity and from receiver, and thickness of inhomogeneity. The curvature of the spherical shell is varied
to study the effects of the shape of inhomogeneous volume element on scattering. 相似文献
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Ivan V. BRAGIN Georgy A. CHELNOKOV Oleg V. CHUDAEV Natalia A. KHARITONOVA Sergey V. VYSOTSKIY 《《地质学报》英文版》2016,90(1):276-284
Studied waters belong to warm(T=30-50℃),alkaline(pH=8.9-9.3),low mineralized(TDS235 mg/1)Na-HCO_3 or Na-SO_4-HCO_3 thermal waters with high content of SiO_2(up to 81 mg/l)and F(up to 3.9 mg/1),occur on modern volcano-tectonic rejuvenated areas of Eastern Sikhote-Alin orogenic belt.Low~3He concentration as well as N_2/O_2 and N_2/Ar ratios exclude influence of deep mantle fluid.New rare earth element data constrain our understandmg of water-rock interaction occurring in the water source region.Meteoric origin of waters is proved by stable isotope values varying from-71‰to-136.1‰and from-10.8‰to-18.8‰forδ~2U andδ~(18)O respectively.REE patterns reflect high pH,resultfing from water-rock interaction and oxidative conditions.Calculations of deep aquifer temperature using Na-K and quartz geothermometers show 116.8-131.1°C and 82.2-125.8℃respectively.Presence of deep faults both with abnormal thermal gradient(~45-50 K/km)define unique geochemical shape of thermal waters of Sikhote-Alin,area,where no present volcanic activity is registered. 相似文献
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地震次生地质灾害风险评估集对态势分析 总被引:2,自引:0,他引:2
5.12四川汶川8级强震引发了大量次生地质灾害,加剧了灾情并严重影响抗震救灾。地震次生地质灾害受多重因素制约,其孕育与致灾过程具有不确定性。利用集对分析原理与方法,对地震次生地质灾害进行同异反态势分析,拟定了风险评估的集对分析同一度、差异度、对立度等指标体系的构建原则与赋值标准,对承灾体系统的不确定性及其作用作了刻画与分析,建立了不同风险分区代表性的集对分析联系度表达式,为地震灾害研究提供了可资借鉴的新思路和技术方法。 相似文献
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下扬子区三叠纪古地理演化 总被引:2,自引:2,他引:0
下扬子区在三叠纪期间接受了早-中三叠世海相碳酸盐沉积、中-晚三叠世海陆交互相和陆相湖沼沉积.沉积相带的空间分布和古地理格局的变迁明显地受到区域构造的控制.区内盆地发育与演化是在华南板块与扬子板块、扬子板块与华北板块相互作用的背景下进行的.早-中三叠世末期的印支运动是下扬子区构造-古地理格局改变的决定性因素,使下扬子海盆闭合,沉积类型由海相沉积变为陆相沉积.下扬子区三叠纪古地理的演化特征也为板块碰撞提供了沉积证据. 相似文献
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Isothermal thermogravimetric experiments have been carried out to determine the reaction kinetics of the dehydration processes
in fuller's earth, a natural Ca-montmorillonite. Dehydration in swelling clays is a complex reaction, and analysis of the
thermogravimetric data using empirical rate equations and time-transformation analysis reveals that the nature of the rate
controlling mechanism is dependent upon both the temperature regime of the sample as well as the extent of reaction. For fuller's
earth, we find that the dehydration kinetics are dominated by a nucleation and growth mechanism at low temperatures and fractions
transformed (stage I), but above 90 °C the last stages of the reaction are diffusion controlled (stage II). The activation
energy for dehydration during stage I is around 35 kJ · mol−1, whereas the removal of water during stage II requires an activation energy of around 50 kJ · mol−1. These two stages of dehydration are associated with primary collapse of the interlayer (stage I) and movement of water that
is hydrated to cations within the interlayer (stage II).
Received: 28 August 1998 / Revised, accepted: 27 January 1999 相似文献