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1.
本文运用伊利石结晶度、绿泥石结晶度、云母b0值和绿泥石地质温度计研究了梵净山前寒武系甚低级变质作用。结果表明经Kisch伊利石结晶度标样校正的伊利石结晶度Kübler指数为0.20~0.99°Δ2θ,绿泥石结晶度árkai指数为0.22~0.63°Δ2θ。由此阐明梵净山前寒武系经历了成岩作用到浅变质作用的影响,迄今依然保留了成岩带、近变质带和浅变质带的岩石记录。成岩岩石具有伊蒙混层特征成岩指示矿物,浅变质带具有钠云母特征变质指示矿物。钾云母(伊利石)b0值范围为:0.9000~0.9045nm;平均0.9018nm,b0值累积频率曲线分布介于典型中压—中低压系列之间,估算的压力为366MPa。峰期变质温度为293~364℃,平均342℃,古变质温压梯度为27℃/km。近变质带界线穿越地层和梵净山背斜轴线,表明甚低级变质作用为成岩-构造运动同期或后期构造增厚引起下部和底部岩石随温压的升高而产生的。 相似文献
2.
湘北杨家坪中新元古宇和下古生界的近变质作用与成岩作用 总被引：1，自引：1，他引：0
运用伊利石结晶度、K云母晶格常数b0、应变值τ、颗粒大小分布与矿物组合分析等低温变质指示数据对湘北杨家坪剖面中晚元古宇和下古生界的近变质作用和成岩作用进行了研究。Kisch国际标样用于校正伊利石结晶度的测定。中晚元古宇伊利石结晶度Kübler指数范围为:0.21~0.24°Δ2θ,而下古生界为0.28~0.67°Δ2θ。表明近变质作用影响了中晚元古宇和部分下古生界。按照Kisch国际标样的成岩/变质界限(0.21~0.38°Δ2θ,CuKα),将剖面划分为北部近变质带和中南部成岩带。由绿泥石化学成分地质温度计估计近变质峰期温度约为260℃。K云母晶格常数b0值变化范围0.9000~0.9045nm,平均为0.9017nm,表明近变质作用处于中压-中低压力范围。近变质带伊利石(主要是中晚元古宇)的多型为2M1型,而成岩带伊利石(主要是下古生界)的多型为2M1+1M混合类型。平均对数粒度与对数方差之积(GLR)称为对数总成熟效应具有不同的两组分布特征即近变质作用区(GLR1.88)与成岩作用区(GLR1.88),这是一个新的发现。后变质作用的构造应力不仅可产生断层,而且可引起矿物的应变,从而导致衍射峰的宽化,使得近变质带伊利石结晶度值次生变大到成岩值范畴。与剖面南部地区(长沙-澧陵-浏阳,黄土店-仙溪,沅古坪)比较,杨家坪剖面中晚元古宇和下古生界经历了中压-中低压近变质作用和成岩作用的影响。这一结果与多数前人认为的"元古宇板溪群处于绿片岩相或亚绿片岩相或低绿片岩相而震旦到下古生界为沉积盖层"的观点不同。 相似文献
3.
长沙—澧陵—浏阳—带冷家溪群及板溪群的甚低级变质作用 总被引：13，自引：5，他引：13
湘东长沙-澧陵-浏阳一带中晚元古宇的冷家溪群及板溪群遭受了区域甚低级变质作用.在本地区所采的＜2μm的样品中,冷家溪群伊利石结晶度的Kübler指数为0.18～0.26°△2θ,板溪群为0.21～0.28°△2θ(Kisch国际标样校正).从而可把本地区冷家溪群的区域变质划归浅变质带和近变质带上部,温度大约为280～400℃.板溪群划归近变质带上部,温度大约为250～300℃.并未普遍达到目前人们认为的绿片岩相或者是低绿片岩相.样品中冷家溪群伊利石(白云母)b0值的范围在0.8999～0.9042 nm,板溪群为0.9018～0.9042nm.由冷家溪群b0频率累积曲线图,得出本区冷家溪群处于较典型的中压区. 相似文献
4.
对巢湖北部地区以碳酸盐岩为主的寒武系—下三叠统海相地层的黏土矿物分析及伊利石结晶度测定的结果表明:伊利石是本区海相地层的主体矿物,平均体积分数为73%。黏土矿物的成岩转化特征表现为蒙皂石的伊利石化。按照伊利石结晶度的成岩-浅变质程度划分,本区寒武系—下三叠统的成岩作用已达到最高成岩阶段。伊利石结晶度的纵向变化总体上可分为上、下两部分:下部寒武系至志留系的结晶度为0.41～0.60°Δ2θ,结晶度与埋深具有一定的相关性,成岩作用是下部地层黏土矿物特征的主控因素;上部泥盆系至下三叠统的结晶度为0.45～0.77°Δ2θ,呈波动变化,蒙皂石连续出现,地层没有被显著埋藏,沉积因素是上部地层黏土矿物特征的主控因素。下三叠统地层中蒙皂石的分布特征以及上泥盆统五通组顶部高岭石的普遍富集具有重要的古气候研究意义。 相似文献
5.
极低级变质作用及其研究方法 总被引：9，自引：2，他引：9
近年来国际上极低级变质作用的研究进展包括综合运用了伊利石结晶度等各项指标 ,将极低级变质带划分为成岩带、近变质带和浅变质带 ,成岩带和近变质带又可进一步划分为低级成岩带、高级成岩带、低级近变质带和高级近变质带 ;研究了伸展背景、阿尔卑斯碰撞背景和增生背景下的极低级变质作用 ;进一步理解了矿物的转变过程 ,建立了变质泥质岩石的矿物反应系列。即变质泥质岩石的二八面体矿物反应系列 ,为蒙皂石—伊 /蒙混层 (I/S)—伊利石—白云母 ;对应变质镁铁质岩石的三八面体矿物反应系列 ,为蒙皂石—绿泥石 /蒙皂石混层 (C/S)—绿泥石。岩石微构造也发生同步变化 ;明确了广泛应用的伊利石结晶度的本质是雏晶大小的一种量度 ,也与晶格应变有关 ,主要受反应动力的控制 ;建立了系统的研究技术方法 ,包括野外采样方法、室内X光衍射法 (XRD)、透射电镜法 (TEM )、地质温度计、地质压力计、岩石学方法、同位素地质学方法等 相似文献
6.
吉林省东部石炭-二叠系伊利石的成因标志 总被引：1，自引：0，他引：1
吉林东部石炭-二叠系主要是一套泥质岩石, 其详细深入的矿物学工作尚不多见。利用JSM-6700F场发射电镜及INCA能谱仪,研究了伊利石的显微形貌和微区成分。采用D/max-2500 X-射线衍射仪,研究了伊利石的结晶度、多型和b0值。结果表明:研究区伊利石结晶度变化于0.26~0.77,平均值为0.44;伊利石（白云母）多型有3种类型,分别为1Md型、1Md+2M1混合型和2M1型;伊利石（白云母）b0值为8.996~9.045,平均值为9.007Å。石炭系伊利石结晶度变化于0.26~0.50,平均值为0.35,主要呈2M1多型,b0平均值为9.011Å,主要是低级近变质带的产物;二叠系伊利石结晶度变化于0.26~0.50,平均值为0.42,主要为1Md+2M1混合型多型,b0平均值为9.004Å,主要为晚期成岩带的产物。 相似文献
7.
黑龙江省上古生界伊利石的成因标志及其地质意义 总被引：2，自引：0，他引：2
采用XRD技术,对黑龙江省上古生界泥质岩石中伊利石结晶度、多型和b值进行了测定,以揭示该区晚古生代极低级变质作用特征。测定结果表明,伊利石结晶度（Kübler指数）主要变化于0.31～0.77 °Δ2θ,伊利石（白云母）b值主要变化于8.983～9.011 A伊利石（白云母）多型为1Md型、1Md+2M1混合型和2M1型。上述伊利石矿物学参数揭示出,该区上古生界泥质岩石主体属于中-低压相晚期成岩带-低级近变质带范畴。进一步的研究表明,伊利石b值和伊利石结晶度存在明显的负相关关系,即随伊利石b值的逐渐增大（压力升高）,伊利石结晶度逐渐减小（温度升高）,暗示伊利石形成于一种正常的与埋深有关的成岩-变质环境,继而揭示出该区上古生界的成岩作用与变质作用是一个统一的连续过程而不是两个相互无关的地质事件。结合区域地质背景和内蒙、吉林等地伊利石的研究成果可以认为,东北地区上古生界并未遭受大规模的绿片岩相区域变质作用,局部出现的某些绿片岩相（或更高级别）的变质岩应是动力变质作用或接触变质作用的产物。 相似文献
8.
本文运用系列黏土矿物学和碳酸盐结构占位的方法研究了蓟县中、新元古界剖面出露的碎屑岩和碳酸盐岩.这些方法包括了伊利石结晶度、绿泥石结晶度、黏土矿物组合、粒度分布、多型、有序度、Mg/Ca离子占位以及地质温压计.结果表明:伊利石结晶度Kübler指数范围为0.37°～1.37°Δ2θ,绿泥石结晶度árkai指数范围为0.31°～2.40°Δ2θ,以及1Md的多型,一致指示本区处于晚期成岩作用影响范围,仅非常有限局部达到了初始变质的状态;黏土矿物组合主要是伊利石、伊蒙混层、绿蒙混层和高岭石;粒度分布范围为8～24 nm,其上界(23～24 nm)达到了NEWMOD计算的理论成岩带/近变质带界限,与结晶度数据一致,也表明了本区处于晚期成岩阶段.白云石有序度的数据表明,本区碳酸盐岩白云石的有序度值范围为0.19～0.99,可分为4个带:甚低级有序带、低级有序带、中级有序带、高级有序带.与川东石炭-二叠系碳酸盐岩相比,中低级有序带有一定的油气前景.本区由西向东,由甚低级有序带变化到高级有序带,白云石有序度升高.估计的成岩作用温度为183～200±20℃,压力为330 MPa,古地热梯度为17～21℃/km. 相似文献
9.
右江盆地三叠纪槽盆相浊流沉积岩系遭受过区域极低级变质作用。依据地质观察和伊利石结晶度、绿泥石-云母堆垛集合体、标志性粘土矿物及白云母(伊利石)b0参数测定资料,阐述了泥质岩石的成岩变质作用经浅层(近)变质作用到浅变质作用的转换特征。变质温度区间为150-350℃,低压类型,具高地温梯度(40-43℃/km).变质级及亚带总体与地层时代及岩层在地层柱中的位置有耦合关系,而与区域变形强度无关。最后指出区域极低级变质作用是印支-燕山构造旋回早期及区域变形前的地质事件,属于地壳伸展构造背景下右江边缘型盆地内部的埋藏型变质作用。 相似文献
10.
11.
Elastic and thermoelastic constants of large single crystals of Ca2MgSi2O7 and Ca2ZnSi2O7 have been derived from ultrasonic resonance frequencies of plane-parallel plates and their shift upon variation of temperature, respectively. In addition, coefficients of thermal expansion and dielectric constants were determined. Both species possess quite similar properties. As observed in other isotypic magnesium and zinc compounds, the mean elastic stiffness and the deviation from the Cauchy relations are significantly larger in the zinc compound, due to a covalent contribution of the Zn–O bond. Positive thermoelastic constants T44 and T66 in Ca2MgSi2O7 allow temperature-independent ultrasonic generators and oscillators to be manufactured. 相似文献
12.
含Ti硅酸盐玻璃在基础科学研究和应用技术开发上均有重要价值,亟需对其进行准确的成分分析,为进一步的科研工作提供重要的数据支撑.对玻璃进行电子探针分析时,由于样品的易损性和其中(Na和K)阳离子在电子束轰击下极易发生迁移和扩散,因此往往需要经过条件实验来确定合适的分析条件,确保样品在该条件下能够保持尽量稳定的状态,才能获... 相似文献
13.
Hydrometallurgical processing and recovery of molybdenum trioxide from spent catalyst 总被引：5，自引：0，他引：5
Kyung Ho Park B. Ramachandra Reddy D. Mohapatra Chul-Woo Nam 《International Journal of Mineral Processing》2006,80(2-4):261-265
Hydrometallurgical processing of spent hydrodesulphurisation (HDS) catalyst for the recovery of molybdenum using sodium carbonate and hydrogen peroxide mixtures was investigated. The results indicated that the recovery of molybdenum was largely dependent on the concentrations of Na2CO3 and H2O2 in the reaction medium, which controls the acidity of the leach liquor and carry over of impurities such as Al, Ni, P, Si and V. Leaching process was exothermic and leaching efficiency of molybdenum decreased with increasing solid to liquid ratio. Large scale leaching of spent catalyst, under optimum conditions: 20% pulp density, 85 g/L Na2CO3, 10 vol.% H2O2 and 1 h reaction, resulted a leaching efficiency of 84% Mo. The obtained leach liquor contained (g/L): Mo — 22.0, Ni — 0.015 and Al — 0.82, P — 1.1, Si — 0.094 and minor quantities of V — 8 mg/L, As and Co — < 1 mg/L. Recovery of Mo from leach solution as MoO3 of 97.30% purity was achieved by ammonium molybdate precipitation method. 相似文献
14.
Classical atomistic simulation techniques have been used to investigate the energies of hydrogen defects in Mg2SiO4 and Mg2GeO4 spinels. Ringwoodite (γ-Mg2SiO4) is considered to be the most abundant mineral in the lower part of the transition zone and can incorporate large amounts
of water in the form of hydroxyls, whereas the germanate spinel (γ-Mg2GeO4) corresponds to a low-pressure structural analogue for ringwoodite. The calculated defect energies indicate that the most
favourable mechanisms for hydrogen incorporation are coupled either with the reduction of ferric iron or with the creation
of tetrahedral vacancies. Hydrogen will go preferentially into tetrahedral vacancies, eventually leading to the formation
of the hydrogarnet defect, before associating with other negatively charged point defects. The presence of isolated hydroxyls
is not expected. The same trend is observed for germanate, and thus γ-Mg2GeO4 could be used as a low-pressure analogue for ringwoodite in studies of water-related defects and their effect on physical
properties. 相似文献
16.
Gianluca Iezzi Mario Tribaudino Giancarlo Della Ventura Fabrizio Nestola Fabio Bellatreccia 《Physics and Chemistry of Minerals》2005,32(7):515-523
The synthetic amphibole Na0.95(Li0.95Mg1.05)Mg5Si8O22(OH)2 was studied in situ at high-T, using IR OH-stretching spectroscopy and synchrotron X-ray powder diffraction. At room-T the sample has P21
/m symmetry, as shown by the FTIR spectrum. It shows in the OH region two well-defined and intense absorptions at 3,748 and
3,712 cm−1, respectively, and two minor bands at 3,667 and 3,687 cm−1. The main bands are assigned to the two independent O–H groups in the primitive structure. The two minor bands evidencing
the presence of small amount of vacant A-site (A□0.05). With increasing T, these bands shift continuously and merge into a unique absorption at high temperature. A change as a function of increasing
T is revealed by the evolution of the refined unit-cell parameters, whose trend shows a transition to C2/m at about 320–330°C. The spontaneous scalar strain, fitted with a tricritical 2–6 Landau potential, gives a T
c of 325(10)°C (β parameter = 0.27). Comparison with the second-order P21
/m ⇔ C2/m phase transition at 255°C for synthetic amphibole ANa0.8B(Na0.8Mg1.2)CMg5Si8O22(OH)2 indicates that the substitution of Na with Li at the B-sites strongly affects the thermodynamic character and the T
c of the phase transition. The comparison of LNMSH amphiboles with cummingtonitic ones shows that the high-T thermodynamic behaviour is affected by A-site occupancy. 相似文献
17.
We present results from low-temperature heat capacity measurements of spinels along the solid solution between MgAl2O4 and MgCr2O4. The data also include new low-temperature heat capacity measurements for MgAl2O4 spinel. Heat capacities were measured between 1.5 and 300 K, and thermochemical functions were derived from the results.
No heat capacity anomaly was observed for MgAl2O4 spinel; however, we observe a low-temperature heat capacity anomaly for Cr-bearing spinels at temperatures below 15 K. From
our data we calculate standard entropies (298.15 K) for Mg(Cr,Al)2O4 spinels. We suggest a standard entropy for MgAl2O4 of 80.9 ± 0.6 J mol−1 K−1. For the solid solution between MgAl2O4 and MgCr2O4, we observe a linear increase of the standard entropies from 80.9 J mol−1 K−1 for MgAl2O4 to 118.3 J mol−1 K−1 for MgCr2O4. 相似文献
18.
The influence on the structure of Fe2+ Mg substitution was studied in synthetic single crystals belonging to the MgCr2O4–FeCr2O4 series produced by flux growth at 900–1200 °C in controlled atmosphere. Samples were analyzed by single-crystal X-ray diffraction, electron microprobe analyses, optical absorption-, infrared- and Mössbauer spectroscopy. The Mössbauer data show that iron occurs almost exclusively as IVFe2+. Only minor Fe3+ (<0.005 apfu) was observed in samples with very low total Fe. Optical absorption spectra show that chromium with few exceptions is present as a trivalent cation at the octahedral site. Additional absorption bands attributable to Cr2+ and Cr3+ at the tetrahedral site are evident in spectra of end-member magnesiochromite and solid-solution crystals with low ferrous contents. Structural parameters a0, u and T–O increase with chromite content, while the M–O bond distance remains nearly constant, with an average value equal to 1.995(1) Å corresponding to the Cr3+ octahedral bond distance. The ideal trend between cell parameter, T–O bond length and Fe2+ content (apfu) is described by the following linear relations: a0=8.3325(5) + 0.0443(8)Fe2+ (Å) and T–O=1.9645(6) + 0.033(1)Fe2+ (Å) Consequently, Fe2+ and Mg tetrahedral bond lengths are equal to 1.998(1) Å and 1.965(1) Å, respectively. 相似文献
19.
The high-pressure behavior of a vanadinite (Pb10(VO4)6Cl2, a = b = 10.3254(5), c = 7.3450(4) Å, space group P63/m), a natural microporous mineral, has been investigated using in-situ HP-synchrotron X-ray powder diffraction up to 7.67 GPa with a diamond anvil cell under hydrostatic conditions. No phase transition has been observed within the pressure range investigated. Axial and volume isothermal Equations of State (EoS) of vanadinite were determined. Fitting the P–V data with a third-order Birch-Murnaghan (BM) EoS, using the data weighted by the uncertainties in P and V, we obtained: V 0 = 681(1) Å3, K 0 = 41(5) GPa, and K′ = 12.5(2.5). The evolution of the lattice constants with P shows a strong anisotropic compression pattern. The axial bulk moduli were calculated with a third-order “linearized” BM-EoS. The EoS parameters are: a 0 = 10.3302(2) Å, K 0(a) = 35(2) GPa and K′(a) = 10(1) for the a-axis; c 0 = 7.3520(3) Å, K 0(c) = 98(4) GPa, and K′(c) = 9(2) for the c-axis (K 0(a):K 0(c) = 1:2.80). Axial and volume Eulerian-finite strain (fe) at different normalized stress (Fe) were calculated. The weighted linear regression through the data points yields the following intercept values: Fe a (0) = 35(2) GPa for the a-axis, Fe c (0) = 98(4) GPa for the c-axis and Fe V (0) = 45(2) GPa for the unit-cell volume. The slope of the regression lines gives rise to K′ values of 10(1) for the a-axis, 9(2) for the c-axis and 11(1) for the unit cell-volume. A comparison between the HP-elastic response of vanadinite and the iso-structural apatite is carried out. The possible reasons of the elastic anisotropy are discussed. 相似文献
20.
Mathematical models of hydrocarbon formation can be used to simulate the natural evolution of different types of organic matter and to make an overall calculation of the amounts of oil and/or gas produced during this evolution. However, such models do not provide any information on the composition of the hydrocarbons formed or on how they evolve during catagenesis.From the kinetic standpoint, the composition of the hydrocarbons formed can be considered to result from the effect of “primary cracking” reactions having a direct effect on kerogen during its evolution as well as from the effect of “secondary cracking” acting on the hydrocarbons formed.This report gives experimental results concerning the “primary cracking” of Types II and III kerogens and their modelling. For this, the hydrocarbons produced have been grouped into four classes (C1, C2–C5, C6–C15 and C15+). Experimental data corresponding to these different classes were obtained by the pyrolysis of kerogens with temperature programming of 4°C/min with continuous analysis, during heating, of the amount of hydrocarbons corresponding to each of these classes.The kinetic parameters of the model were optimized on the basis of the results obtained. This model represents the first step in the creation of a more sophisticated mathematical model to be capable of simulating the formation of different hydrocarbon classes during the thermal history of sediments. The second step being the adjustment of the kinetic parameters of “secondary cracking”. 相似文献