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91.
桃江县板溪锑矿床地质特征及成矿构造分析 总被引:1,自引:0,他引:1
桃江县板溪锑矿,主要开采2号矿脉,它赋存在上元古界板溪群五强溪组上段,由中矿脉、东支脉和西盲脉组成,矿石矿物主要是辉锑矿,平均厚度0.40 m,平均品位Sb 25.48%,属燕山期中低温热液型锑矿床。矿区成矿构造V_2和V_(2-1)断裂,成矿前显张扭性,成矿期转化为压扭性质,西盲脉,则充填V_(2-2)断裂派生的“多”字型构造。它们为矿区富厚矿体提供了主要成矿空间,展示了构造与矿床的密切成生联系。 相似文献
92.
本文对陕西潼关石英脉型金矿床中石英的比重、比磁化率、晶胞参数、化学成分和包裹体等特征进行了比较详细的研究,重点用红外光谱研究了石英中包裹体的 CO_2和 H_2O 相对光密度与含金性关系。 相似文献
93.
为了了解水对受力岩石的宏观力学效应,在MTS电液伺服材料试验系统上,对不同饱水度的砂岩、花岗闪长岩、灰岩和大理岩进行了单轴压缩试验,取得了这几种岩石的单轴抗压强度和弹性模量随饱水度变化的定量结果.结果表明,水对受力岩石的力学效应与岩石中的含水状态是密切相关的,自然状态的砂岩、花岗闪长岩浸水后,其峰值强度和弹性模量随饱水度的增加而迅速衰减,当饱水度达到某一定值时,这两种岩石的峰值强度和弹性模量基本稳定下来;文中用函数Y=Aexp(-Bx)+C对实验结果进行了最小二乘法拟合.实验中求得水饱和状态和自然状态砂岩的泊松比并没有明显差异,说明在宏观上水对该种岩石受力变形的作用是各向同性的.通过10-5/s和10-4/s两种不同应变率试验,发现水对受力岩石的力学效应具有时间依赖性,这一特点说明仅从有效应力原理来考虑水对受力岩石的力学效应是不够的,而应考虑应力腐蚀这样复杂的过程.此外,大理岩的试验结果表明,水对受力的碳酸盐类岩石的作用机理是一个值得进一步探讨的问题,它与水对受力的含SiO2类岩石相比,可能存在差异. 相似文献
94.
人工合成硅灰石的发光性质与发光机理的初步研究 总被引:2,自引:0,他引:2
在254nm紫外光照激发条件下,对人工合成掺入不同激活离子的低温TC型和高温型假硅灰石的发光性质进行了实验测定,从微观原子能量谱项讨论了在全的硅灰石基质中Eu^3+和Gd^3+的发光机理,分析了Bi^3+对Eu^3+与Pb^2+对Mn^2+的敏化发光条件,初步探讨了掺放Eu^3+的高温型假硅灰石发光强度减弱的原因。 相似文献
95.
Interpolated grids of coal bed thickness are being considered for use in a proposed method for taxation of coal in the state of West Virginia (United States). To assess the origin and magnitude of possible inaccuracies in calculated coal tonnage, we used conditional simulation to generate equiprobable realizations of net coal thickness for two coals on a 7
min topographic quadrangle, and a third coal in a second quadrangle. Coals differed in average thickness and proportion of original coal that had been removed by erosion; all three coals crop out in the study area. Coal tonnage was calculated for each realization and for each interpolated grid for actual and artificial property parcels, and differences were summarized as graphs of percent difference between tonnage calculated from the grid and average tonnage from simulations. Coal in individual parcels was considered minable for valuation purposes if average thickness in each parcel exceeded 30 inches. Results of this study show that over 75% of the parcels are classified correctly as minable or unminable based on interpolation grids of coal bed thickness. Although between 80 and 90% of the tonnages differ by less than 20% between interpolated values and simulated values, a nonlinear conditional bias might exist in estimation of coal tonnage from interpolated thickness, such that tonnage is underestimated where coal is thin, and overestimated where coal is thick. The largest percent differences occur for parcels that are small in area, although because of the small quantities of coal in question, bias is small on an absolute scale for these parcels. For a given parcel size, maximum apparent overestimation of coal tonnage occurs in parcels with an average coal bed thickness near the minable cutoff of 30 in. Conditional bias in tonnage for parcels having a coal thickness exceeding the cutoff by 10 in. or more is constant for two of the three coals studied, and increases slightly with average thickness for the third coal. 相似文献
96.
硬土—软岩工程地质信息管理分析系统及其应用 总被引:3,自引:1,他引:2
在中国大规模的工程建设实践中,人们积累了大量与硬土-软岩有关的工程经验和测试数据,总结这些测试结果并用现代计算机技术进行自动化管理是十分必要的,作者以中国科学院地质与地球物理研究所工程地质力学开放研究实验室多年来的室内试验结果为基础,研制开发了“硬土-软岩工程地质信息管理分析系统(HRGISM)”软件,实现了岩土工程地质信息资源管理的自动化和可视化,并在信息管理的基础上强化了试验数据分析和工程特性预测功能,本文简要地介绍了HRGIMS系统的主要功能和实际应用。 相似文献
97.
98.
介绍滇中红层形成的地质历史背景,红层分布范围,主要地层岩性及区内地质构造。重点讨论滇中红层特别是红层软岩的岩体原生结构,及后期受构造改造的岩体结构特性,岩体风化特性,岩体水理作用特性,岩体物理力学性质等四方面的工程地质特性。 相似文献
99.
Andrew G. Tomkins 《Mineralium Deposita》2007,42(6):627-637
The relative importance of mechanical re-mobilisation, hydrothermal dissolution and re-precipitation, and sulphide melting
in controlling redistribution of metals during concurrent metamorphism and deformation is evaluated at the middle amphibolite
facies Montauban deposit in Canada. As at many other deposits, ductile deformation was important in driving mechanical re-mobilisation
of massive sulphides from limb regions into hinge regions of large-scale folds and is thus the most important for controlling
the economics of Pb and Zn distribution. Two possible stages of hydrothermally driven re-mobilisation are discussed, each
of which produces characteristically different alteration assemblages. Prograde hydrothermal re-mobilisation is driven by
pyrite de-sulphidation and concurrent chlorite dehydration and is thus an internally driven process. At Montauban, the H2S-rich fluid generated through this process allowed re-mobilisation of gold into the wall rock, where it was deposited in
response to sulphidation of Fe Mg silicates. Retrograde hydrothermal re-mobilisation is an externally driven process, whereby
large volumes of fluids from outside the deposit may dissolve and re-precipitate metals, and cause hydration of silicate minerals.
This second hydrothermally driven process is not recognised at Montauban. Sulphide melting occurred as temperatures neared
the peak metamorphic conditions. Melting initiated in the massive sulphides through arsenopyrite breakdown, and a small volume
of melt was subsequently re-mobilised into the wall rock. Trace element partitioning and fractional crystallisation of this
melt generated a precious metal-rich fractionate, which remained mobile until well after peak metamorphism. Thus, prograde
hydrothermal re-mobilisation and sulphide melting were the most important mechanisms for controlling the distribution of Au
and Ag. 相似文献
100.
Wenjun Yong E. Dachs A. C. Withers E. J. Essene 《Physics and Chemistry of Minerals》2007,34(2):121-127
A multi-anvil device was used to synthesize 24 mg of pure γ-Fe2SiO4 crystals at 8.5 GPa and 1,273 K. The low-temperature heat capacity (C
p) of γ-Fe2SiO4 was measured between 5 and 303 K using the heat capacity option of a physical properties measurement system. The measured
heat capacity data show a broad λ-transition at 11.8 K. The difference in the C
p between fayalite and γ-Fe2SiO4 is reduced as the temperature increases in the range of 50–300 K. The gap in C
p data between 300 and 350 K of γ-Fe2SiO4 is an impediment to calculation of a precise C
p equation above 298 K that can be used for phase equilibrium calculations at high temperatures and high pressures. The C
p and entropy of γ-Fe2SiO4 at standard temperature and pressure (S°298) are 131.1 ± 0.6 and 140.2 ± 0.4 J mol−1 K−1, respectively. The Gibbs free energy at standard pressure and temperature (ΔG°
f,298) is calculated to be −1,369.3 ± 2.7 J mol−1 based on the new entropy data. The phase boundary for the fayalite–γ-Fe2SiO4 transition at 298 K based on current thermodynamic data is located at 2.4 ± 0.6 GPa with a slope of 25.4 bars/K, consistent
with extrapolated results of previous experimental studies. 相似文献