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THE DETERMINATION OF THE EQUATION OF STATE OF MOLTEN SILICATES AT HIGH PRESSURES USING SHOCK-WAVE TECHNIQUES.

机译:利用冲击波技术确定高压下熔融硅酸盐的状态方程。

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摘要

Shock wave (Hugoniot) equation-of-state experiments have been carried out on molten silicates in the petrologically important system CaMgSi(,2)O(,6)-CaAl(,2)Si(,2)O(,8) via the projectile impact method. An RF heating technique was developed to heat silicate samples contained in pure Mo containers to the necessary high initial temperatures (up to 1773 K). Thermocouple techniques, a refractory sample holding system and optical shutter systems, were developed to allow utilization of a propellant gun apparatus at impact velocities ranging from 1.0 to 2.5 km sec('-1) corresponding to shock pressures of 4 to 40 GPa. The methodology for taking into account the effect of the Mo container in measuring the equation of state of the molten silicate is explicitly derived.;The measured equation of state data for molten diopside is used in conjunction with other thermochemical data to constrain the diopside solidus via the Clausius-Clapeyron equation at pressures up to 20 GPa. The present data are consistent with measured fusion curve data of others to 5 GPa. Above (TURN)10GPa, a marked shallowing of the solidus is predicted as the difference in volume between crystalline and molten diopside in equilibrium approaches zero.;Comparison of the results for molten diopside with those from the intermediate composition indicates that the liquids exhibit ideal mixing behavior with respect to volume to within (+OR-)2% up to (TURN)40GPa. Gradual changes in coordination of Al('3+) and Si('4+) from tetrahedral at low pressures to octahedral at high pressures are believed to occur during compression of these materials. The integrated compressibility as reflected in the values of K(,S) and K' is related to the proportion of tetrahedrally coordinated cations at low pressure, and the volume at (TURN)40 GPa is from 100-110% of that of a mixture of the dense, high-pressure phases MgSiO(,3) (perovskite), CaSiO(,3) (perovskite), Al(,2)O(,3) (corundum) and SiO(,2) (stishovite).;Important petrological implications of our results include: (1) basic to ultrabasic melts become denser than olivine- and pyroxene-rich mantle at pressures of 6-10 GPa, and (2) there is a maximum depth from which basaltic melt can rise buoyantly within terrestrial planetary interiors.;Results on molten diopside (CaMgSi(,2)O(,6)), anorthite (CaAl(,2)Si(,2)O(,8)) and an intermediate composition (36 mole % CaAl(,2)Si(,2)O(,8), 64 mole % CaMgSi(,2)O(,6):An(,0.36)Di(,0.64)) are presented. Reduction of the Hugoniot data for these materials to third-order Birch-Murnaghan isentropes yields 1 atm bulk moduli (K(,S)) in the range 18-24 GPa which are in good agreement with bulk moduli recently measured by ultrasonic methods at 1 atm and similar temperatures. The pressure derivatives of bulk modulus (K') vary from 5-7. Shock temperature calculations for An(,0.36)Di(,0.64) indicate temperatures of 2400-2600 K at (TURN)25 GPa. The Hugoniot states are believed to lie metastably in the liquid field on the basis of measured bulk modulus, calculated Hugoniot density of a solid of the same composition and estimated crystallization times.
机译:在岩石学上重要的系统CaMgSi(,2)O(,6)-CaAl(,2)Si(,2)O(,8)中对熔融硅酸盐进行了冲击波(Hugoniot)状态方程实验弹丸撞击法。开发了一种射频加热技术,将纯Mo容器中容纳的硅酸盐样品加热到必要的高初始温度(最高1773 K)。开发了热电偶技术,耐火样品保持系统和光学百叶窗系统,以允许在1.0至2.5 km sec('-1)的冲击速度(对应于4至40 GPa的冲击压力)下使用推进剂枪装置。明确推导了考虑到Mo容器在测量熔融硅酸盐的状态方程中的影响的方法。;熔融的透辉石的状态数据的测量方程与其他热化学数据结合使用,通过以下方式约束透辉石的固相线压力高达20 GPa时的Clausius-Clapeyron方程。当前数据与其他测量到的5 GPa的融合曲线数据一致。高于(TURN)10GPa时,由于在平衡状态下结晶和熔融透辉石之间的体积差异接近零,预计固相线会显着变浅;熔融透辉石与中间成分的结果比较表明液体显示出理想的混合相对于体积(+ OR-)2%以内(TURN)40GPa的行为。据信,在这些材料的压缩过程中,Al('3+)和Si('4+)的配位从低压的四面体到高压的八面体逐渐发生变化。反映在K(,S)和K'值上的整体压缩率与低压下四面体配位阳离子的比例有关,(TURN)40 GPa时的体积为混合物体积的100-110% MgSiO(,3)(钙钛矿),CaSiO(,3)(钙钛矿),Al(,2)O(,3)(刚玉)和SiO(,2)(水辉石)高压相。我们研究结果的重要岩石学意义包括:(1)在6-10 GPa的压力下,超碱性熔体的碱性比富橄榄石和辉石的地幔致密,并且(2)玄武质熔体在其中可浮起的最大深度地球熔融物;熔融的透辉石(CaMgSi(,2)O(,6)),钙长石(CaAl(,2)Si(,2)O(,8))和中间成分(36摩尔%CaAl( ,2)Si(,2)O(,8),提出了64摩尔%的CaMgSi(,2)O(,6):An(,0.36)Di(,0.64))。将这些材料的Hugoniot数据还原为三阶Birch-Murnaghan等熵,可以得到18-24 GPa范围内的1 atm体积模量(K(,S)),这与最近通过超声方法在1处测得的体积模量很好atm和类似的温度。体积模量(K')的压力导数为5-7。 An(,0.36)Di(,0.64)的冲击温度计算表明(TURN)25 GPa时的温度为2400-2600 K.根据测得的体积模量,计算出的相同组成的固体的Hugoniot密度和估计的结晶时间,据信Hugoniot状态稳定地位于液相中。

著录项

  • 作者

    RIGDEN, SALLY MIRANDA.;

  • 作者单位

    California Institute of Technology.;

  • 授予单位 California Institute of Technology.;
  • 学科 Geophysics.
  • 学位 Ph.D.
  • 年度 1986
  • 页码 146 p.
  • 总页数 146
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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