板片俯冲过程中Co、Ni的分布及迁移特征——以西南天山为例

在板片俯冲过程中,基性洋壳、下伏蛇纹石化岩石圈地幔和覆盖在俯冲洋壳上的大洋沉积物在不同深度会依次发生板片脱水作用和沉积物熔融,形成的俯冲带熔/流体可携带某些元素交代地幔楔,进而通过弧岩浆作用返回地壳。同时,俯冲板片内不同组分之间也会发生化学成分的迁移和交换,并最终进入深部地幔,造成地幔不均一性和不同程度壳幔相互作用。本文报道了我国西南天山典型高压-超高压变质带中蛇纹岩、辉石岩、绿片岩、蓝片岩和榴辉岩内各矿物相的主量元素及Cu、Co、Ni含量数据。结果表明,除辉石岩中透辉石的Cu含量较高(1.26×10^-6～76.9×10^-6)外,其它硅酸盐矿物的Cu含量均在1.0×10^-6～10.0×10^-6左右;而Co和Ni在不同岩性及不同矿物之间显示较大的含量差异：蛇纹岩中蛇纹石的Co和Ni含量分别为22.6×10^-6～49.6×10^-6和482×10^-6～1097×10^-6,榴辉岩中绿辉石的Co和Ni含量分别为6.0×10...     

雅鲁藏布江蛇绿岩中橄榄石的位错构造及上地幔流变状态

本文通过对雅鲁藏布江蛇绿岩中橄榄石的透射电子显微分析（TEM）和变形参数测算,划分出3个应变带,即强应变带、过渡型应变带和弱应变带,并详细地研究了它们的岩石结构、位错构造、变形机制和流变状态。镁铁质糜棱岩组成的强应变带中橄榄石发育亚颗粒和位错网络,具有低自由位错密度(10⁷～10⁸cm^-2),是在温度为850～950℃、压力10～13kbar、差异应力2～3MPa、应变速率为10^-16～10^-17s^-1、粘度10²²～10²³Pa.s,大致相当于35～40km的岩石圈深部由位错机制控制的深层剪切流变作用形成的。     

秦岭-大别山壳幔岩石高温高压下的电性特征

首次报导了秦岭-大别山壳幔岩石高温高压下电导率的测定结果。该区中上地壳主要代表岩石(角闪岩、绢云母石英片岩、千枚岩等)在10^-25km的温压条件下,含水矿物出现脱水会引起电导率值升高,认为这是该区出现高导层体的主要原因;中下地壳代表性岩石(片麻岩、麻粒岩、榴辉岩等)由于石英从α相向β相转变,会导致电导率值(σ)下降。在下地壳的温压条件下电导率值一般为10^-2到10^-3S·m^-1;上地幔的代表性岩石由于组成矿物较为基性,电导率值比下地壳高,从0.1到1S·m^-1。     

蚀变洋壳玄武岩俯冲过程中含碳矿物相变质演化及脱碳作用的研究

俯冲作用是连接地表系统和地球深部系统的最为关键的地质过程,其对研究地球深部碳循环具有重要的意义。俯冲洋壳岩石圈中的碳主要存储在沉积物、蚀变洋壳玄武岩以及蛇纹岩中。俯冲变质作用过程含碳岩石的变质演化控制着其中含碳矿物相的转变及碳迁移过程。本文选取了蚀变洋壳玄武岩进行相平衡模拟,来研究其含碳矿物相的变质演化过程。计算结果表明,变质玄武岩体系中的碳酸盐矿物之间的转变反应除了受压力控制之外,还受到温度和体系中铁含量的影响。随着压力的升高蚀变玄武岩中碳酸盐矿物会发生方解石/文石-白云石-菱镁矿的转变,但在高压/超高压条件下,温度的升高可以使菱镁矿转变成白云石。碳酸盐矿物中的铁含量受到体系中铁含量的影响,白云石和菱镁矿中的铁含量随着体系中铁含量的增加而增加。在水不饱和条件下,洋壳不管是沿着低温还是高温地热梯度线俯冲到岛弧深度,蚀变玄武岩体系几乎都不发生脱碳作用。然而在水饱和条件下,当洋壳沿着高温以及哥斯达黎加地热梯度线俯冲到岛弧深度时,蚀变玄武岩体系中的碳几乎可以全部脱出去。蚀变玄武岩体系中水含量的增加可以促进体系的脱碳作用。     

甘肃北山红石山地区晚石炭世英云闪长岩锆石U- Pb年龄、地球化学特征及构造意义

笔者等以出露于红石山—百合山蛇绿混杂岩带南侧的英云闪长岩体为研究对象,通过野外地质调查和岩石学、地球化学、锆石LA-ICP-MS U-Pb年代学研究,探讨其成因、构造环境及红石山洋俯冲消亡过程。岩石地球化学研究表明,红石山南英云闪长岩体富硅(SiO₂=63.95%～66.22%)、高铝(Al₂O₃=15.31%～16.61%)、富钠(Na₂O=3.73%～4.33%)、低钾(K₂O=1.00%～1.85%),相对高锶(Sr=246.0×10^-6～417.0×10^-6)、低钇(Y=8.83×10^-6～11.80×10^-6),富集Rb、Sr等大离子亲石元素和LREE,亏损Nb、Ta、Ti、P等高场强元素,HREE相对亏损,无明显Eu异常。岩石学和岩石地球化学特征表明,为俯冲洋壳脱水熔融的产物。锆石LA-ICP-MS U-Pb测年表明,红石山南英云闪长岩体的形成年龄为306.9～309.9 Ma,...     

高温高压下叶蜡石脱水电学性质的阻抗谱分析

在1.0、2 .0GPa和873～12 2 3K的温压条件下,借助于12 6 0阻抗增益相位分析仪测定了叶蜡石的电导率,并用阻抗谱原理分析了其微观导电机制。实验结果表明:样品的电导率对频率具有很强的依赖性;电阻率随着温度的升高而减小,电导率随着温度升高而增大,logσ与1/T之间符合Arrenhius线性关系;叶蜡石在1.0GPa和2 .0GPa的压力下脱水温度分别为10 74K和110 1K。根据本次获得的电导率实验结果并结合前人对滑石族所做的工作,得出了与前人不同的结论:滑石族矿物脱水电导率曲线出现了转折点。     

高温高压下叶蜡石脱水电导率实验

在压力为1.0～4.0 GPa、温度为873～1 223 K下采用Sarltron-1260阻抗/增益-相位阻抗谱分析仪测定了叶蜡石的电导率.实验结果表明,电导率与温度间的关系符合Arrenhius关系式;叶蜡石的脱水引起电导率的突然变化,使电导率急剧上升;脱水前,电导率随着压力增大而减小,其导电机制为电子导电;脱水后,电导率随着压力增大而增大,其导电机制为离子导电.     

变质改造型关键金属矿——富集Li-Rb-Cs-Tl-Ga的云母片岩

关键金属矿产是国际上最近提出的资源概念,对战略性新兴产业的发展至关重要,但认知程度较低。洛扎岩浆-变质杂岩体位于喜马拉雅带东部,侵位于藏南拆离系内。在岩体东北侧,云母片岩被含电气石淡色花岗岩捕虏。云母片岩主要由金云母、绿泥石和少量黑云母组成。从全岩地球化学成分来看,云母片岩具有含量较高的Al₂O₃(13.38%～14.32%)、K₂O(6.09%～9.66%)、FeO^*(27.11%～30.09%)、MgO(15.25%～17.21%)、TiO₂(0.09%～0.26%),富集关键金属Li(650×10^-6～1 031×10^-6)、Rb(1 649×10^-6～2 773×10^-6)、Cs(98×10^-6～229×10^-6)、Tl(5.7×10^-6～12.1×10^-6)、Ga(121×10^-6     

方解石在不同水环境中的溶解与沉淀作用

方解石的溶解与沉淀是各种岩溶地质作用的基础,但对其在不同水环境条件下的溶解过程和溶解度有待深入研究。文章通过实验研究了天然方解石(CaCO₃)在不同水环境中的溶解作用。结果表明,方解石在纯净水、空气饱和水、CO₂饱和水、初始pH=3的溶液和初始pH=9的溶液中溶解时,Ca浓度随着溶解时间的增加呈现缓慢升高并趋于稳定,在溶解4 080 h后达到0.4444～0.4696 mmol·L^-1、0.402 0～0.415 4 mmol·L^-1、0.573 9-0.659 7 mmol·L^-1、1.098 1 mmol·L^-1和0.448 9 mmol·L^-1;方解石(CaCO₃)在纯净水中溶解时溶度积(K_sp)为10^-8.48±0.08～10^-8.48±0.13,吉布斯生成自由能ΔG_f^o[CaCO₃     

滇西北衙富碱斑岩的特征及成因

提供了与滇西北衙大型金矿床密切相关的富碱斑岩的主量元素及稀土和微量元素的分析数据,对富碱斑岩的成因、起源条件和源区类型进行了讨论。研究表明,北衙地区的富碱斑岩具有较高的SiO₂(w(SiO₂)＞68％)和Al₂O₃(w(Al₂O₃)=13.45％～15.22％),具有富集Sr(w(Sr)=365×10^-6～930×10^-6),亏损HREE(w(Yb)=0.64×10^-6～1.17×10^-6)和Y(w(Y)=7.17×10^-6～12.25×10^-6),较高的w(Sr)/w(Y)、w(La)N/w(Yb)N比值,无明显的负Eu异常等特征,显示了与埃达克岩的某些相似性。然而,富碱斑岩低的w(MgO)、w(Cr)和w(Ni),又与典型的埃达克岩有所不同。富碱斑岩产出的地质背景及岩石学和地球化学特征表明,富碱斑岩并非起源于俯冲的大洋板片,而是源于加厚地壳的底部,源区为榴辉岩相岩石。富碱斑岩显著富集Rb、Ba、Th、K,可能与俯冲大陆板片的脱水作用和流体的交代作用有关。产生富碱斑岩岩浆的动力学机制,与印度大陆板块和扬子大陆板块对“三江”的相向俯冲、金沙江-红河断裂带的走滑拉分及其诱发的软流圈上涌和流体交代作用有关。     

Viscosity of albite melt at high pressure and high temperature

 The viscosity of albite (NaAlSi₃O₈) melt was measured at high pressure by the in situ falling-sphere method using a high-resolution X-ray CCD camera and a large-volume multianvil apparatus installed at SPring-8. This system enabled us to conduct in situ viscosity measurements more accurately than that using the conventional technique at pressures of up to several gigapascals and viscosity in the order of 10⁰ Pa s. The viscosity of albite melt is 5.8 Pa s at 2.6 GPa and 2.2 Pa s at 5.3 GPa and 1973 K. Experiments at 1873 and 1973 K show that the decrease in viscosity continues to 5.3 GPa. The activation energy for viscosity is estimated to be 316(8) kJ mol⁻¹ at 3.3 GPa. Molecular dynamics simulations suggest that a gradual decrease in viscosity of albite melt at high pressure may be explained by structural changes such as an increase in the coordination number of aluminum in the melt. Received: 6 January 2001 / Accepted: 27 August 2001     

Electrical conductivity of K-feldspar at high temperature and high pressure

Electrical conductivity measurements on dry polycrystalline K-feldspar were performed at 1.0 to 3.0 GPa and 873 to 1,173 K with a multi-anvil high-pressure apparatus and the Solartron-1260 Impedance/Gain Phase Analyzer in the frequency range of 10^?1 to 10⁶ Hz. At each temperature the complex impedance displays a perfect semi-circular arc that represents the grain-interior conduction. Under the experimental conditions, electrical conductivity exponentially increases with increasing temperature and slightly decreases with increasing pressure; however, the effect of pressure on the conductivity is less pronounced than that of temperature. The activation enthalpy decreases slightly from 0.99 to 1.02 eV with increasing pressure, and the activation energy and activation volume for K-feldspar are 0.98 eV and 1.46?±?0.17 cm³/mol, respectively. According to these Arrhenius parameters, ionic conduction is proposed to be the dominant conduction mechanism in K-feldspar at high temperatures and pressures, and potassium ions are the charge carriers transporting by an interstitial mechanism. The diffusion coefficient of potassium at high temperatures was calculated from our conductivity data on K-feldspar using Nernst–Einstein equation, and the results were compared with the previous experimental results.     

X-ray diffraction study of magnesite at high pressure and high temperature

 P–V–T measurements on magnesite MgCO₃ have been carried out at high pressure and high temperature up to 8.6 GPa and 1285 K, using a DIA-type, cubic-anvil apparatus (SAM-85) in conjunction with in situ synchrotron X-ray powder diffraction. Precise volumes are obtained by the use of data collected above 873 K on heating and in the entire cooling cycle to minimize non-hydrostatic stress. From these data, the equation-of-state parameters are derived from various approaches based on the Birch-Murnaghan equation of state and on the relevant thermodynamic relations. With K′₀ fixed at 4, we obtain K₀=103(1) GPa, α(K⁻¹)=3.15(17)×10⁻⁵ +2.32(28)×10⁻⁸ T, (∂K_T/∂T)_P=−0.021(2) GPaK⁻¹, (dα/∂P)_T=−1.81×10⁻⁶ GPa⁻¹K⁻¹ and (∂K_T/∂T)_V= −0.007(1) GPaK⁻¹; whereas the third-order Birch-Murnaghan equation of state with K′₀ as an adjustable parameter yields the following values: K₀=108(3) GPa, K′₀=2.33(94), α(K⁻¹)=3.08(16)×10⁻⁵+2.05(27) ×10⁻⁸ T, (∂K_T/∂T)_P=−0.017(1) GPaK⁻¹, (dα/∂P)_T= −1.41×10⁻⁶ GPa⁻¹K⁻¹ and (∂K_T/∂T)_V=−0.008(1) GPaK⁻¹. Within the investigated P–T range, thermal pressure for magnesite increases linearly with temperature and is pressure (or volume) dependent. The present measurements of room-temperature bulk modulus, of its pressure derivative, and of the extrapolated zero-pressure volumes at high temperatures, are in agreement with previous single-crystal study and ultrasonic measurements, whereas (∂K_T/∂T)_P, (∂α/∂P)_T and (∂K_T/∂T)_V are determined for the first time in this compound. Using this new equation of state, thermodynamic calculations for the reactions (1) magnesite=periclase+CO₂ and (2) magnesite+enstatite=forsterite+CO₂ are consistent with existing experimental phase equilibrium data. Received September 28, 1995/Revised, accepted May 22, 1996     

铁橄榄石高温高压流变性的实验研究

通过高温高压实验研究了铁橄榄石集合体的流变性.首先,利用高精度的Paterson气体介质变形装置对铁橄榄石集合体Fe2SiO4进行了高温三轴压缩蠕变试验.变形试验条件为:温度1273～1423K,围压300MPa,差应力10～250MPa,应变率10-7～10-4s-1,试件的最大变形量不超过20%.利用三维非线性拟合方法对蠕变试验数据进行分析,得到铁橄榄石集合体的微观变形机制为扩散域和位错域,扩散域的应力指数为1左右.位错蠕变域中,干燥铁橄榄石集合体的应力指数为5.4.活化能为781kJ/mol;含水铁橄榄石集合体的应力指数为3.4,活化能为516kJ/mol.实验结果表明,含水时铁橄榄石的流变强度比干燥时小一个数量级.将实验结果与铁橄榄石单晶的强度进行对比,发现铁橄榄石集合体的流变强度比铁橄榄石单晶的强度高.从而得到了铁橄榄石集合体高温高压流变性(强度)的初步试验结果.     

玄武岩的高温高压实验研究

玄武岩及其高温高压相—榴辉岩的相组合,经历了长期的地质作用,反映出一定的时空条件。从高温高压实验矿物学,实验岩石学入手,对于以相组合出现的某些化学体系进行平衡条件研究,可揭示此类岩石形成的物理化学环境,并有助于阐明地球内部的物理状态、组成成分以及活动过程。     

The Electrical Conductivity of Gabbro at High Temperature and High Pressure

The electric conductivity of gabbro has been measured at 1.0 - 2.0 GPa and 320-700℃, and the conduction mechanism has been analyzed in terms of the impedance spectra.Experimental results indicated that the electric conductivity depends on the frequency of alternative current. Impedance arcs representing the conduction mechanism of grain interiors are displayed in the complex impedance plane, and the mechanism is dominated at high pressure.These arcs occur over the range of 102 - k× 105 Hz (k is the positive integer from 1 to 9). On the basis of our results and previous work, it is concluded that gabbro cannot form any high conductivity layer (HCL) in the middle-lower crust.     

耐高温高压复合保温管研究

耐高温高压复合保温管主要解决超高温高压环境下钻孔测量问题。为攻克超高温高压环境下真空绝热保温、高压密封等关键技术,研究的耐高温高压复合保温管为“超高温钻孔测量仪”提供一种耐高温承压管,使用环境温度可达270 ℃,压力120 MPa。通过室内测试与现场应用,说明其满足超高温高压要求,可应用于高温地热能钻探工程、干热岩钻探工程、科学钻探工程、深部矿产资源勘探和深部油气资源勘探等工程中,为超高温大深度钻井测量提供技术支撑。     

存储式高温高压钻孔测温仪的研制与应用

为解决大于200 ℃高温环境下的测温难题,为高温地热和干热岩资源勘查提供技术支撑,利用铂电阻测温技术和真空绝热保温技术研发了存储式高温高压钻孔测温仪。该仪器设计适用工作环境温度为300 ℃,耐水压100 MPa,主要用于高温高压环境下的钻孔测温。在广东惠州惠热1井和青海共和GH-01井进行了实测应用,满足目前钻遇到的孔底温度的测温要求。     

Thermodynamic properties of San Carlos olivine at high temperature and high pressure

In this study, the thermal expansion and heat capacity of San Carlos olivine under high temperature and high pressure are reported. Combining accurate sound velocity data under different P–T conditions with density and heat capacity data at ambient pressure, the density, adiabatic bulk modulus, shear modulus, and most importantly, thermal expansion and heat capacity, of San Carlos are extracted to 14 GPa by a numerical procedure using classic thermodynamic relationships. These data are in agreement with published findings. To estimate the temperature gradient in the upper mantle, we also report the fitting equations of thermal expansion and heat capacity of San Carlos olivine as a function of both temperature and pressure to the P–T condition of the 410 km discontinuity, which provide the thermodynamic properties with increasing depth in the Earth’s interior.     

Phonon density of states in iron at high pressures and high temperatures

The phonon density of states (DOS) in iron has been measured in situ by nuclear resonance inelastic X-ray scattering (NRIXS) at high pressures and high temperatures in a resistively heated diamond anvil cell. The DOS data provide a variety of thermodynamic and elastic parameters essential for characterizing iron at depth in the Earth interior, such as average sound velocity, Debye temperature, atomic mean square displacement, average kinetic energy, vibrational entropy and specific heat. The NRIXS data were collected at 6, 20, and 29 GPa and at temperatures up to 920 K. Temperatures were directly determined from the measured spectra by the ratio of intensities of the phonon creation/annihilation side bands that are determined only by the Boltzmann factor. The change of the DOS caused by the structural transition from -Fe to -Fe is small and not resolvable within the experimental precision. However, the phonon energies in -Fe are clearly shifted to lower values with respect to - and -Fe. The temperature dependence of derived thermodynamic parameters is presented and compared with those obtained by Debyes model. The Debye temperatures that best describe the data decrease slightly with increasing temperature.