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1.
玄武岩的高温高压实验研究 总被引：4，自引：0，他引：4
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。 N.L.Bowen早在1928年曾根据高温下的实验 相似文献
2.
高温高压实验岩石学可有效地验证埃达克质岩浆的成因,是研究埃达克质岩成因的一项重要手段。实验研究表明,在水不饱和条件下,微量元素含量合适的中基性岩石在高温高压下的脱水部分熔融都有可能得到类似于埃达克质成分的熔体,其残留相为含有石榴子石、缺失斜长石的岩石组合。侧重于实验产物微量元素的研究将是今后实验岩石学的一个发展方向。 相似文献
3.
长石在高温高压条件下的物理化学行为 总被引：2，自引：0，他引：2
长石是地学上非常重要的矿物之一。它有可能随着板块俯冲而进入地球深部,因此它在高温高压条件下的相行为以及物理化学性质对地球深部地球动力学研究非常有意义。本文总结了长石端员组份(钾、钠、钙长石)以及其固溶体系列已知的高温、高压实验数据,并绘制成相图。已有的研究成果显示:这三种端员组份在高压下的相行为有较大差异,并产生了许多只在高温高压条件下稳定的相如K-Holl-I、K-Holl-II、CF、CAS及CaPv等。由这些高压相构成的具有长石成分的不同相组合的密度在约5~23GPa的压力范围内超过地幔岩的密度,因此这些相组合可以主动俯冲到上地幔的深处。另一方面,已有研究表明,这些高压相对碱金属及碱土金属在地幔中的赋存状态有着非常重要的影响。 相似文献
4.
高温高压微束衍射实验进展及其地学应用 总被引：6，自引：6，他引：6
同步辐射X射线微束衍射技术与静态高压装置(包括金刚石压砧设备和大腔体压力机设备)结合运用是研究高温高压下物质晶体结构、相变等的有效方法。金刚石压砧高温高压实验技术的发展体现在:在产生极端高温高压的同时,获得准确的实验温度压力值,采用充装气体传压介质等方法减小压力梯度,采用激光双面加温技术和改进激光光路以减小样品径向和轴向的温度梯度。大腔体压力机高温高压实验技术的发展主要表现在产生更高的实验压力,以及测试过程中使样品在一定幅度摆动以消除晶体生长和择优取向对衍射数据的影响。同步辐射X射线微束衍射技术的发展主要表现在更高亮度和更宽能量范围的同步辐射光源的使用、X射线聚焦技术的发展,以及角色散X射线衍射测试技术的进步。介绍了近年来高温高压微束衍射实验在地球科学领域所取得的一些最新进展,包括硅酸盐超钙钛矿的实验发现,铁的高温高压相变及熔融曲线、SiO2 超斯石英相变、橄榄石尖晶石相—超尖晶石相转变压力的精确测定等研究结果;认为硅酸盐超钙钛矿的进一步深入研究,水对地球深部矿物岩石力学性质及熔融行为的影响,高温高压下物质的化学反应性和地球深部元素的地球化学行为等,是今后高温高压实验研究的重要方向。 相似文献
5.
地球深部物质科学——在静高压大腔体实验研究方面的某些进展 总被引：1，自引：0，他引：1
介绍近年来使用静态超高压大腔体实验技术 ,在模拟地球内部的高温高压条件下 ,对地球物质进行的若干物理和化学性质的实验研究。高压同时高温条件下多种岩石样品的弹性波速就位测量揭示出物质的声软化现象和振幅效应 ;高温高压下陨石和岩石的熔融结晶实验发现了陨石硅酸盐相的不混溶现象以及玄武岩熔体结构的变化 ,在玄武岩转变为榴辉岩的实验中观测到了刚玉相 ;在高温高压水的实验中 ,发现了冰 Ⅶ 的亚稳相和熔融前效应以及超临界水及其稀溶液的一些新性质。这些实验结果为探索地球深部物质的性质和状态以及迁移和演化提供了新的依据。 相似文献
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辉长岩的高压部分熔融实验研究 总被引：8，自引：5，他引：3
利用天然含水辉长岩在１．５～３．０ＧＰａ,９００℃～１４４０℃条件下进行了高温高压部分熔融实验,系统地分析了辉长岩部分熔融后实验产物的岩石学、矿物学、地球化学特征。获得了１）辉长岩的高压熔融曲线,２）辉长岩在不同压力下熔融时,残留相矿物组合及期间矿物相转变与熔融液相成分（相当于安山岩浆）特征。认识了辉长岩与榴辉岩相间的相变关系;辉长岩－榴辉岩－安山岩之间的内在联系以及高温榴辉岩的可能成因。 相似文献
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在高温高压条件下进行了铁、锌及铅的硫化物在氯化物溶液中溶解度的实验研究。实验中pH是用石英二长岩加白云母的硅酸盐组合控制的,fs_2和fo_2则用黄铁矿+磁黄铁矿+磁铁矿组合控制。实验表明,影响贱金属浓度的主要因素有温度、氯化物总浓度和压力。正如所预料的那样,高温及高氯 相似文献
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华中高压－超高压变质富铝岩石为陆壳岩石经变质而成，其典型的岩石类型为蓝晶石黄玉石英岩。矿物温压计估算其ｐ－Ｔ条件为Ｔ＝７００℃，ｐ＝１．２ＧＰａ；高温高压实验结果表明，蓝晶石＋黄玉组合在Ｔ＝１０００～１２００℃，Ｐ＝３．１～３．７７ＧＰａ范围内可以稳定存在，是高压－超高压变质作用产物。在蓝晶石石英岩中发现柯石英及柯石英假象，区域上其它岩石组合也有高压－超高压变质作用的证据。变质富铝岩石为榴辉岩相变质作用产物，从而证明陆壳岩石可以经历＞２．０ＧＰａ的变质压力条件。 相似文献
10.
选用吉林陨石富金属相,在3GPa压力、405℃～1850℃温度下,采用两种组装方式进行实验。并与先前肇东陨石全岩样的高压熔融实验进行比较。三个系列实验结果的综合对比表明,高温高压下球粒陨石中金属和硫化物经历了固相扩散、熔融和熔体聚集的过程。固相扩散使金属与硫化物彼此结合,形成了若干个小的FeNi-FeNiS二元系,使其在比Fe-Ni熔点低的温度下熔融形成Fe-Ni-S熔体。该熔体与硅酸盐熔体不相混溶,因而发生自身的合并与聚集。其合并和聚集速率与硅酸盐粘度有关。实验过程中陨石里的磷酸盐矿物可以被还原,使单质P进入金属硫化物相。这些实验结果为讨论地核的形成机理提供了依据。 相似文献
11.
A. Suzuki E. Ohtani K. Funakoshi H. Terasaki T. Kubo 《Physics and Chemistry of Minerals》2002,29(3):159-165
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 相似文献
12.
Haiying Hu Lidong Dai Heping Li Jianjun Jiang Keshi Hui 《Mineralogy and Petrology》2014,108(5):609-618
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. 相似文献
13.
J. Zhang I. Martinez F. Guyot P. Gillet S. K. Saxena 《Physics and Chemistry of Minerals》1997,24(2):122-130
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, (∂KT/∂T)P=−0.021(2) GPaK−1, (dα/∂P)T=−1.81×10−6 GPa−1K−1 and (∂KT/∂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, (∂KT/∂T)P=−0.017(1) GPaK−1, (dα/∂P)T= −1.41×10−6 GPa−1K−1 and (∂KT/∂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 (∂KT/∂T)P, (∂α/∂P)T and (∂KT/∂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 相似文献
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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. 相似文献
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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. 相似文献
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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. 相似文献
19.
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. 相似文献
20.
En-Ping Huang Eugene Huang Shu-Cheng Yu Yen-Hua Chen Jiann-Shing Lee Jiann-Neng Fang 《Physics and Chemistry of Minerals》2010,37(9):593-600
Kerogen samples were treated at temperatures and pressures up to 25–600°C and ~9 GPa, respectively. In situ micro-Raman spectroscopy
was used to measure the systematic changes in the first-order Raman spectral features during the process of temperature or
pressure increment. Three Raman bands, D1, D2, and G bands, were examined to characterize the structural and chemical changes
of kerogen at high temperatures and pressures. We found that the wavenumbers of D1, D2 and G bands showed a linear variation
with both temperature and pressure. Therefore, a correlation between R1 and R2 and the peak temperature in regionally metamorphosed
rocks cannot be applied to this work. This result implies that the G band may serve as a temperature or pressure indicator
during the promotion of maturation of kerogen. Kerogen possesses reversible properties in contrast with the natural samples
recovered from the field suffered from prolonged thermal history during regional metamorphism. 相似文献