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131.
裂隙型单斜介质中弹性系数的计算及波的传播特性研究 总被引:3,自引:1,他引:3
根据Hudson等关于裂隙介质弹性系数计算的扰动理论及Bond变换矩阵原理,给出了各向同性介质中含多组垂直裂隙时等效弹性系数的计算方法。计算了含两组斜交的垂直裂隙形成的单斜各向异性介质中的等效弹性系数,并根据Christoffel方程推导、得出水平面内平面波传播的相速度和群速度随方位变化的特性。 相似文献
132.
自然界的大多数造岩矿的是由两种或多种组分混合而成的固溶体。因此,在矿物,岩石和矿床等地质体的平衡热力学研究中不可避免地要涉及固溶体矿物热力学地为的问题。河南省西峡县杨乃沟红柱石矿泥质片岩中仅出现红柱石而没有蓝晶石和夕线石,红柱石矿物包裹体测温结果为420-600℃。通过矿物共生平衡p-t曲线所计算出的片岩形成温度和压力条件也应位于上述岩石学和岩相学等特征所限定的范围内。以此为基础,通过构筑矿物共生p-t平衡曲线的方法,对片岩中若干固溶体矿物理想性/非理想性问题进行了研究。其中斜长石必须以非理想固溶体处理,而石榴子石,黑云母和白云母视作理想固溶体的计算结果同片岩的岩石学和岩相学等特征相一致。 相似文献
133.
为了计算高温,高压和高密度流体的热力学性质,提出了一个具有19个参数的维里型状态方程,其中参数与温度间的函数关系采用由Sutherland位能函数导出的维里系数近似式。除临界点附近以外,在已报道的pVT数据所覆盖的大部分超临界区域内,该方程均可适用。用该方程对H2O,CH4,H2,CO2,CO和O2等流体pVT关系的计算结果令人满意,其中pVT上限分别为:91-610GPa,1.6-11.0cm^3/mol,4000-5000K。计算体积的平均偏 小于0.8%,最大偏差小于5.4%。 相似文献
134.
为探讨高原牌70kN和进口120,210kN瓷绝缘子的成分和结构性能,中采用原子吸收光谱(AAS)和X射线衍射(XRD)方法,对三类产品进行了检测。结果表明,有效成分除K2O外,70kN和210kN的SiO2,Al2O3,Fe2O3含量接近,主晶相基本相同,有刚玉,莫来石、石英和长石等;结晶相总量:70kN35%,120kN40%,210kN48%,这表明机械强度愈大,结晶相含量愈高,只需调整70kN原样的部分成分,粒度和工艺,即生产出高等级(如210kN)瓷绝缘子。 相似文献
135.
高温高压下电解质溶液热力学性质的研究不仅对探讨地球内部流体的作用具有重要意义,而且在很多实际工业过程中也都有广泛应用。本综述了近10年来高温高压下电解质溶液热力学参数的实验测量和理论计算的进展,实验设备还有待进一步的改进和完善,以获得更高温度和压力下的数据,理论计算不仅有待于实验的发展,也与溶液的结构理论密切相关。 相似文献
136.
河北矾山燕山期侵入岩地球化学特征及成因 总被引:8,自引:0,他引:8
河北矾山地区燕山期侵入岩可分为早、晚两期。早期(中侏罗世-晚侏罗世)侵入岩主要由二长闪长岩、石英二长闪长岩、石英二长岩、正长岩构成,以高钾钙碱性岩系列岩石为主;SiO2=53.58%-60.57%,Al2O3=16.16%-17.23%,Na2O K2O=5.76%-8.96%,K2O=2.25%-4.55%,Na2O/K2O=1.14-1.56;ACNK=0.72-0.86,NKA=0.47-0.77;Eu^*/Eu=0.80-0.95,轻稀土富集,重稀土和Nb、Ta、Hf、Ti亏损,相对低Zr、Rb和Rb/Sr,但高Sr和Sr/Y,具有埃达史质岩石质岩石的部分特征。晚期(白垩纪)侵入岩由碱长石英正长岩、石英正长岩、石英二长岩、碱工花岗岩、钾长花岗岩构成,以钾玄岩系列岩石为主;比早期岩石富SiO2,低Al2O3、富Na2O K2O和K2O,但低Na2O/K2O;ACNK=0.82-1.07,NKA=0.77-0.92;Eu^*/Eu=0.65-1.00,轻稀土富集,重稀土和Nb、Ta、Hf、Ti亏损,相对高Zr、Rb和Rb/Sr,但低Sr和Sr/Y。矾山地区早期侵入岩的形成可能与伊泽奈崎(Izanaqi)板块向欧亚大陆板块的俯冲所导致的挤压增厚有关;晚期侵入岩可能形成于拉张环境中。 相似文献
137.
Analogue study of particle segregation in pyroclastic density currents, with implications for the emplacement mechanisms of large ignimbrites 总被引:3,自引:0,他引:3
Abstract Analogue flume experiments were conducted to investigate the transport and sedimentation behaviour of turbulent pyroclastic density currents. The experimental currents were scaled approximately to the natural environment in three ways: (1) they were fully turbulent; (2) they had a very wide range of particle sizes and associated Rouse numbers (the ratio of particle settling velocity to effective turbulent eddy velocity in the current); and (3) they contained particles of two different densities. Two sets of surge‐type experiments were conducted in a 5 m long, water‐filled lock‐exchange flume at five different volumetric particle concentrations from 0·6% to 23%. In one set (one‐component experiments), the currents contained just dense particles; in the other set (two‐component experiments), they contained both light and dense particles in equal volume proportions. In both sets of experiments, the population of each component had a log‐normal size distribution. In the two‐component experiments, the size range of the light particle population was selected in order to be in hydrodynamic equivalence with that of the dense particles. Dense particles were normally graded, both vertically and downstream, in the deposits from both sets of experiments. The mass loading (normalized to the initial mass of the suspension) and grain size of the dense component in the deposits decreased with distance from the reservoir and were insensitive to initial total particle concentration in the currents. On the other hand, in the two‐component experiments, the light particles were extremely sensitive to concentration. They were deposited in hydrodynamic equivalence with the dense particles from dilute currents, but were segregated efficiently at concentrations higher than a few per cent. With increasing particle concentration, the large, light particles were carried progressively further down the flume because of buoyancy effects. Deposits from the high‐concentration currents exhibited reverse vertical grading of the large, light particles. Efficient segregation of the light component was observed even if the bulk density of the current was less than that of the light particles. In both sets of experiments, marked inflexions in the rate of downstream decline in mass loading and maximum grain size of the dense component can be attributed to the presence of two different particle settling regimes in the flow: (1) particles with Rouse numbers >2·5, which did not respond to the turbulence and settled rapidly; and (2) particles with Rouse numbers <2·5, which followed the turbulent eddies and settled slowly. The results are applied to the transport and sedimentation dynamics of pyroclastic density currents that generate large, widespread ignimbrites. Field data fail to reveal significant departures from aerodynamic equivalence between pumice and lithic clasts in three such ignimbrites: the particulate loads of some large ignimbrites are transported principally in turbulent suspensions of low concentration. In some ignimbrites, the well‐developed inflexions in curves of maximum lithic (ML) size vs. distance can be attributed to the existence of distinct high and low Rouse number particle settling regimes that mark the transition from an overcharged state to one in which the residual particulate load is transported more effectively by turbulence. 相似文献
138.
An experimental study of grain scale melt segregation mechanisms in two common crustal rock types 总被引:3,自引:0,他引:3
Creation of pathways for melt to migrate from its source is the necessary first step for transport of magma to the upper crust. To test the role of different dehydration‐melting reactions in the development of permeability during partial melting and deformation in the crust, we experimentally deformed two common crustal rock types. A muscovite‐biotite metapelite and a biotite gneiss were deformed at conditions below, at and above their fluid‐absent solidus. For the metapelite, temperatures ranged between 650 and 800 °C at Pc=700 MPa to investigate the muscovite‐dehydration melting reaction. For the biotite gneiss, temperatures ranged between 850 and 950 °C at Pc=1000 MPa to explore biotite dehydration‐melting under lower crustal conditions. Deformation for both sets of experiments was performed at the same strain rate (ε.) 1.37×10?5 s?1. In the presence of deformation, the positive ΔV and associated high dilational strain of the muscovite dehydration‐melting reaction produces an increase in melt pore pressure with partial melting of the metapelite. In contrast, the biotite dehydration‐melting reaction is not associated with a large dilational strain and during deformation and partial melting of the biotite gneiss melt pore pressure builds more gradually. Due to the different rates in pore pressure increase, melt‐enhanced deformation microstructures reflect the different dehydration melting reactions themselves. Permeability development in the two rocks differs because grain boundaries control melt distribution to a greater extent in the gneiss. Muscovite‐dehydration melting may develop melt pathways at low melt fractions due to a larger volume of melt, in comparison with biotite‐dehydration melting, generated at the solidus. This may be a viable physical mechanism in which rapid melt segregation from a metapelitic source rock can occur. Alternatively, the results from the gneiss experiments suggest continual draining of biotite‐derived magma from the lower crust with melt migration paths controlled by structural anisotropies in the protolith. 相似文献
139.
An automated strategy for calculation of phase diagram sections and retrieval of rock properties as a function of physical conditions 总被引:9,自引:0,他引:9
We formulate an algorithm for the calculation of stable phase relations of a system with constrained bulk composition as a function of its environmental variables. The basis of this algorithm is the approximate representation of the free energy composition surfaces of solution phases by inscribed polyhedra. This representation leads to discretization of high variance phase fields into a continuous mesh of smaller polygonal fields within which the composition and physical properties of the phases are uniquely determined. The resulting phase diagram sections are useful for understanding the phase relations of complex metamorphic systems and for applications in which it is necessary to establish the variations in rock properties such as density, seismic velocities and volatile‐content through a metamorphic cycle. The algorithm has been implemented within a computer program that is general with respect to both the choice of variables and the number of components and phases possible in a system, and is independent of the structure of the equations of state used to describe the phases of the system. 相似文献
140.
在兴安金石金矿外围 4号分散流异常区 ,通过地电化学提取金测量法 ,查明测区存在 5个走向规模小于 5 0 m的金异常区 ,W( Au) 最大值为 72 .4× 10 - 9,高出背景值十几倍 ,并藉综合土壤吸附汞测量 ,高精度磁测和激发极化法等多种物化探方法来确定这些异常区的地质、地球化学和地球物理特征 ,提出金矿成矿的有利部位在金的地电提取高异常区、高汞量异常区、高磁性异常区、低视电阻率异常区和中等视极化率异常区的“三高一低一中”的找矿模式。确定测区的北北东角 (右下角 )一带具备有利的金矿成矿条件 相似文献