硅灰石矿物发光材料的人工合成研究

对硅灰石矿物发光材料进行了人工合成研究，在合成试样中，分别掺入少量Ｅｕ＾３＋，Ｇｄ＾３＋，Ｐｂ＾２＋，Ｍｎ＾２＋等激活剂，于１０００℃或１１８０℃条件下分别通入Ｈ２Ｓ（ｇ），Ｈ２Ｏ（ｇ）以及用ＮＨ３，Ｈ２Ｏ吸收ＣＯ２（ｇ）等方法进行合成低温ＴＣ型三斜硅灰石和高温型假硅灰石，合成产物通过扫描电镜、Ｘ射线衍射和红外光谱实验，对合成过程中温度高低，时间长短、冷却快慢、降低温度合成高温型假硅灰石的方法进行     

金在碱性富硅热液中溶解和迁移的实验研究

实验测定了金在碱性富硅溶液中的溶解度，并标定了Ａｕ与ＳｉＯ２之间的配合关系Ａｕ＾＋Ｈ２ＳｉＯ＾－４＝ＡｕＨ３ＳｉＯ＾０４在８０￣２５０℃的温度范围内，其平衡常数为ｌｇＫ＝－１．９８８９＋１００８５。１８／Ｔ（Ｔ为绝对温度）各温度下的平衡常数值与Ａｕ－ＨＣｌ－ＳｉＯ２－Ｈ２Ｏ体系中得到的结果一致。它表明溶液在酸性和碱性条件下，ＳｉＯ２均作为配位体，与Ａｕ形成ＡｕＨ３ＳｉＯ＾０４在热液中溶解、迁移。Ａ     

2，4－二溴－6－羧基苯重氮氨基偶氮苯光度法测定痕量铊的研究

研究了新试剂２，４－二溴－６－羧基苯重氮氨基偶氮苯与Ｔｌ（Ⅲ）的高灵敏显色反应。在非离子表面活性剂ＴｒｉｔｏｎＸ－１００存在下，于ｐＨ１０．５的ＮＨ＿３·Ｈ＿２Ｏ－ＮＨ＿４Ｃｌ缓冲介质中，Ｔｌ（Ⅲ’）与该试剂生成红色配合物，其配合物的最大吸收波长位于５２０ｎｍ处，摩尔吸光系数为１．８３×１０￣５Ｌ·ｍｏｌ￣－１·ｃｍ￣－１。Ｔｌ（Ⅲ’）量在０～０．６４μｇ／ｍｌ范围内符合比尔定律。方法用于废水中痕量Ｔｌ的测定，结果与其它方法结果相符。测定工业废水及粉煤灰中痕量Ｔｌ的ＲＳＤ（ｎ＝６）在１．６％～３．２％范围。     

泡塑吸附分离ICP—AES测定地质样品中痕量铊

采用泡塑吸附Ｔｌ（Ⅱ）。试验了Ｂｒ２水和Ｈ２Ｏ２两种氧化剂对Ｔｌ（Ⅰ）的氧化效果。采用动态吸附，静态解脱Ｔｌ（Ⅱ）。拟定了泡塑吸附－ＩＣＰ－ＡＥＳ测定地质试样中痕量的分析方法。用于土壤。岩石、水系沉积物及多金属矿石等国家一级标准物质分析，结果吻合较好。     

高岭石—莫来石反应系列：^27Al和^29SiMAS NMR研究

根据艰我国八个不同成因和特征的高岭土样品在４５０－１４５０℃热处理产物的ＭＡＳ ＮＭＲ谱和ＸＲＤ，ＩＲ，ＤＴＡ等研究结果，结合有关资料讨论了高岭石－莫来石反应序列的几个重要问题：１．高岭石的结构，尤其是五配位铝；２．９８０℃放热峰后的高温相是γ－Ａｌ２Ｏ３而不是Ａｌ－Ｓｉ尖晶石；３．对于莫来石化过程，认为初始莫来石８５０－９５０℃变高岭石形成，二次莫来石由分凝的ＳｉＯ２和γ－Ａｌ２Ｏ３在１２００－     

Cr^2＋在橄榄石,斜方辉石和尖晶石中溶解度的实验研究

为了研究Ｃｒ＾２＋在橄榄石、斜方辉石和尖晶石中的溶解度及其在各相间的分配，在压力为０－２．８８ＧＰａ和温度为１１００－１４５０℃的条件下，于ＭｇＯ－ＳｉＯ２－Ｃｒ－Ｏ体系中完成了一系列实验。实验起始成分由高纯度的ＭｇＯ、ＳｉＯ２、Ｃｒ２Ｏ３和Ｃｒ混合得到。通过Ｃｒ２Ｏ３和Ｃｒ等化学混合得到所需的ＣｒＯ，且加有过量（５０％）的Ｃｒ，使得实验产物和金属Ｃｒ保持平衡。此外，还加入占起始混合物重量１０％的     

胶东台上金矿成矿机制模拟实验研究

模拟实验研究表明，台上金矿床的成矿机制为：胶东群地层重熔形成滦家河花岗岩岩浆时，初始浆为几乎均匀的熔体相；随着结晶成岩作用的进行，由于局部岩浆结晶分异作用，产生富Ｋ＾＋，Ｎａ＾２＾＋，Ｃａ＾２＾＋，Ｍｇ＾２＾＋，Ｆ＾－，Ｃｌ＾－，Ｓ＾２＾－，ＣＯ３＾２＾－及挥发份ＣＯ２，ＣＯ，Ｈ２Ｏ等的流体相，并不断从已结晶矿物及残熔体中，以［Ａｕ（ＨＳ）２］＾－，［Ａｕ（ＨＳ）Ｓ］＾２＾－，ＡｕＣｌ４］＾－等络     

含水氯化物体系中金和银的相对溶解度测定

文章叙述了用Ａｕ－Ａｇ合金测定Ａｕ和Ａｇ溶解度及讨论Ａｕ的热液行为的意义和方法。实验结果指出：在３００℃，ｆｏ２在１０＾－３５￣１０＾１４间，ΣＣ１＝３．０ｍｏｌ／ｋｇ和有含银矿物存在时，Ａｕ－Ａｇ系列与含水氯化物热液反应，Ａｕ－Ａｇ系列中纯Ａｕ的溶解度最高，中间组分的溶解度随ＸＡｕ的增加而升高，而银的溶解度随ＸＡｇ的变化不明显，但随ΣＣ１＾－浓度的增加而升高，在含银相存在时，金和银总是趋向于形成     

硫化物吸附金属离子的实验研究：——Ⅱ类型

合成ＰｂＳ、ＺｎＳ对金属离子Ａｇ＾＋、Ｃｕ＾２＋、Ｃｄ＾２＋、Ｚｎ＾２＋、Ｆｅ＾２＋、Ｍｎ＾２＋、Ｍｇ＾２＋、Ｓｂ＾２＋和Ｂｉ＾３＋的吸附等温线（５０℃）研究表明，其可分为Ａ、Ｂ、Ｃ三类：Ａ类，线性型，即吸附量随吸附离子浓度增加而呈线性上升，并表现出百分之百吸附，属于此类的吸附有ＰｂＳ对Ａｇ＾＋、Ｃｕ＾２＋离子吸附和ＺｎＳ对Ａｇ＾＋、Ｃｕ＾２＋、Ｃｄ＾２＋离子的吸附；Ｂ类，朗谬尔型，即随吸附离子的     

痕量银与meso－四（对－磺酸基苯基）卟啉显色反应的研究

研究了Ａｇ（Ｉ）与ｍｅｓｏ－四（对－磺酸基苯基）叶琳的光催化显色反应。在ｐＨｌ０的缓冲溶液中形成稳定的Ａｇ（Ｉ）－ＴＰＰＳ＿４－ＣＴＭＡＢ三元配合物，其最大吸收波长为４２６ｎｍ，组成为Ａｇ（１）ＴＰＰＳ＿４：ＣＴＭＡＢ＝１：１：２。表观摩尔吸光系数为２．７９×ｌ０￣５Ｌ·ｍｏｌ￣－１·ｃｍ￣－１，Ａｇ（１）的浓度在０～０．２μｇ／ｍｌ内符合比尔定律。基于此建立的测Ａｇ（Ｉ）方法灵敏度高，结合巯基棉分离干扰，可用于矿物中Ａｇ（Ｉ）的测定。     

交互四元体系Li~+,Mg~(2+)//SO_4~(2-),B_4O_7~(2-)-H_2O 288K时相平衡研究

采用等温溶解平衡法研究了288K时Li+,Mg2+//SO42-,B4O72--H2O四元体系的固液相平衡关系,测定了该四元体系在288K时平衡液相的溶解度和密度。依据实验测定的平衡溶解度数据及对应的平衡固相,绘制了该四元体系的平衡相图及密度组成图。研究结果表明:交互四元体系Li+,Mg2+//SO42-,B4O27--H2O288K时平衡相图中有2个共饱点,5条单变量曲线,4个结晶区对应的平衡固相分别为Li2B4O7.3H2O,Li2SO4.H2O,MgB4O7.9H2O和MgSO4.7H2O。     

http://www.sciencedirect.com/science/article/pii/S1674987114001601

Data from a migmatised metapelite raft enclosed within charnockite provide quantitative constraints on the pressure-temperature-time[P-T-t) evolution of the Nagercoil Block at the southernmost tip of peninsular India.An inferred peak metamorphic assemblage of garnet,K-feldspar.sillimanite,plagioclase,magnetite,ilmenite,spinel and melt is consistent with peak metamorphic pressures of 6-8 kbar and temperatures in excess of 900℃.Subsequent growth of cordierite and biotite record high-temperature retrograde decompression to around 5 kbar and 800 C.SHRIMP U-Pb dating of magmatic zircon cores suggests that the sedimentary protoliths were in part derived from felsic igneous rocks with Palaeoproterozoic crystallisation ages.New growth of metamorphic zircon on the rims of detrital grains constrains the onset of melt crystallisation,and the minimum age of the metamorphic peak,to around560 Ma.The data suggest two stages of monazite growth.The first generation of REE-enriched monazite grew during partial melting along the prograde path at around 570 Ma via the incongruent breakdown of apatite.Relatively REE-depleted rims,which have a pronounced negative europium anomaly,grew during melt crystallisation along the retrograde path at around 535 Ma.Our data show the rocks remained at suprasolidus temperatures for at least 35 million years and probably much longer,supporting a long-lived high-grade metamorphic history.The metamorphic conditions,timing and duration of the implied clockwise P-T-t path are similar to that previously established for other regions in peninsular India during the Ediacaran to Cambrian assembly of that part of the Gondwanan supercontinent.     

Phase relations in the systems Cu2S-PbS-Bi2S3 and Ag2S-PbS-Bi2S3 and their mineral assemblages

The phase diagrams of the systems Cu₂S-PbS-Bi₂S₃ and Ag₂S-PbS-Bi₂S₃ have been investigated in the present study. The paper is concerned with the complete solid solution between bismuthtite and aikinite above 300°C in the system Cu₂S-PbS-Bi₂S₃. The synthetic phases CuBi₃S₅ and Cu₃Bi₅S₉ have their solid solution ranges in the ternary system with 9 and 26 mole% PbS at maximum, respectively. A complete solid solution between PbS and AgBiS₂ divides the phase diagram of the system Ag₂S-PbS-Bi₂S₃ into two parts: Bi-rich and Ag-rich. All sulfosalt minerals and solid solutions, including pavonite ss, lillianite ss, heyovskyite and benjaminite are on the Bi-rich side. And divarant relations were found between pavonite ss -lillianite ss, benjaminite and bismuthtite as well as between lillianite ss -bismuthtite and galenobismutite. Synthetic experiments using LiCl-KCl flux technique show that when a minor amount of copper (less lwt.%) is added in, many of Ag-and Pb-bismuth sulfosalt minerals, for example, vikingite (Ag₅Pb₈Bi₁₃S₃₀), are synthesized successively, particularly at 400°C. So is heyrovskyite, which has a solid solution range with 3.7 mole% Cu₂S at maximum in the system Cu₂S-PbS-Bi₂S₃.     

http://www.sciencedirect.com/science/article/pii/S1674987110000149

The structural stability of manganese titanate MnTiO3 at high pressure was investigated by X-ray diffraction and Raman spectroscopy with diamond anvil cells. Ilmenite-type MnTiO3 is stable at least to 26.6 GPa, and lithium niobate type MnTiO3 reversibly transforms at room temperature to perovskite at 2.0 GPa. Bulk moduli (K300) of ilmenite, lithium niobate and perovskite are 174(4) GPa, 179(8) GPa, and 208(5) GPa, respectively (at fixed first pressure derivative K′ = 4). The Grüneisen parameter γ has been estimated to be 1.28 for ilmenite and 1.75 for perovskite. In ilmenite phase, TiO6 octahedra become more regular with increasing pressure. In perovskite phase structural distortion increases with pressure increase.     

Minerals and calculated low-temperature phase equilibria in the pseudoternary system Tl2S-As2S3-Sb2S3

Summary The experimental determination of phase relations in the pseudoternary system Tl₂ S-As₂S₃-Sb₂S₃ below 200°C is practically impossible, especially so under dry condensed conditions. As thallium sulfosalts are naturally formed at low temperatures equilibrium phase assemblages at 100 and 200°C were calculated by application of thermochemical approximations for the free enthalpies of formation of the sulfosalts. A comparison of the calculated conode configurations with the results of syntheses under dry condensed conditions at 200°C yielded good agreement between experiment and calculations.

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Minerale und Phasenbeziehungen im pseudoternären System Tl₂S-As₂S₃-Sb₂S₃ bei tiefen Temperaturen

Zusammenfassung Die Ableitung der Phasenbeziehungen im pseudoternären System Tl₂S-As₂S₃-Sb₂S₃ für Temperaturen unterhalb 200°C, insbesondere unter trockenen Bedingungen, ist auf experimentellem Weg praktisch nicht möglich. Da die Thalliumsulfosalze als tieftemperierte Mineralbildungen anzusehen sind, wurden die stabilen Gleichgewichtsassoziationen bei 100 und 200°C unter Verwendung thermodynamischer Näherungen für die freie Bildungsenthalpie der Sulfosalze berechnet. Ein Vergleich der berechneten Konodenverläufe mit den Ergebnissen von Versuchen unter trocken kondensierten Bedingungen bei 200°C ergab gute Übereinstimmung zwischen Experiment und Berechnung.

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With 1 Figure     

High pressure elasticity and phase transformation in brucite, Mg(OH)2

The first pressure derivatives of the second-order elastic constants have been calculated for brucite, Mg(OH)₂ from the second- and third-order elastic constants. The deformation theory and finite strain elasticity theory have been used to obtain the second- and third-order elastic constants of Mg(OH)₂ from the strain energy of the lattice. The strain energy ϕ is calculated by taking into account the interactions up to third nearest neighbors in the Mg(OH)₂ lattice. ϕ is then compared with the strain dependent lattice energy from continuum model approximation to obtain the expressions of elastic constants. The complete set of six second-order elastic constants C _IJ of brucite exhibits large anisotropy. Since C ₃₃ (= 21.6 GPa), which corresponds to the strength of the material along the c-axis direction, is less than the longitudinal mode C ₁₁ (= 156.7 GPa), the interlayer binding forces are weaker than the binding forces along the basal plane of Mg(OH)₂. The 14 nonvanishing components of the third-order elastic constants, C _IJK , of brucite have been obtained. All the C _IJK of brucite are negative except the values of C ₁₁₄ (= 230.36 GPa), C ₁₂₄ (= 75.45 GPa) and C ₁₃₄ (= 36.98 GPa). The absolute values of the C _IJK are, in general, one order of magnitude greater than the C _IJ ’s in the Mg(OH)₂ system as usually expected for a crystalline material. To our knowledge, no previous data are available to compare the pressure derivatives of brucite. The pressure derivatives of the two components viz., C ₁₄ and C ₃₃ become negative indicating an elastic instability in brucite while under pressure. This may be related to the phase transition of brucite largely involving rearrangements of H atoms revealed in the Raman spectroscopic, powder neutron diffraction and synchrotron X-ray diffraction studies.     

http://www.sciencedirect.com/science/article/pii/S1674987111000272

We present here a thermodynamic model for predicting multi-phase equilibrium of methane hydrate liquid and vapor phases under conditions of different temperature,pressure,salinity and pore sizes.The model is based on the 1959 van der Waals—Platteeuw model,angle-dependent ab initio intermolecular potentials,the DMW-92 equation of state and Pitzer theory.Comparison with all available experimental data shows that this model can accurately predict the effects of temperature,pressure, salinity and capillary r...     

High-pressure phase transformations in the MgFe2O4 and Fe2O3–MgSiO3 systems

 The crystal structure of MgFe₂O₄ was investigated by in situ X-ray diffraction at high pressure, using YAG laser annealing in a diamond anvil cell. Magnesioferrite undergoes a phase transformation at about 25 GPa, which leads to a CaMn₂O₄-type polymorph about 8% denser, as determined using Rietveld analysis. The consequences of the occurrence of this dense MgFe₂O₄ form on the high-pressure phase transformations in the (MgSi)_0.75(Fe^III)_0.5O₃ system were investigated. After laser annealing at about 20 GPa, we observe decomposition to two phases: stishovite and a spinel-derived structure with orthorhombic symmetry and probably intermediate composition between MgFe₂O₄ and Mg₂SiO₄. At pressures above 35 GPa, we observe recombination of these products to a single phase with Pbnm perovskite structure. We thus conclude for the formation of Mg₃Fe₂Si₃O₁₂ perovskite. Received: 27 March 2000 / Accepted: 1 October 2000     

煤矿瓦斯中H_2S气体的吸附特性及其对治理的影响

基于新疆和山西气煤及瘦煤对H_2S、CH_4和N_2的平衡水条件下的等温吸附实验及Langmuir模型和D-A模型对实验数据的模拟结果,来研究煤矿瓦斯中H_2S气体的吸附特性及其影响因素,并探讨其与H_2S异常矿井的治理关系。结果显示:不同于CH_4和N_2在煤中主要以微孔吸附为主(90%以上),煤中H_2S气体的微孔吸附量仅占Langmuir最大吸附量的36.26%~57.21%,平均为45.99%;气体分子本身的性质是影响煤中H_2S吸附的主要因素,尤其分子直径是影响H_2S气体V_0/V_L远小于CH_4和N2的这种现象的主要原因,也是造成微孔中H_2S气体难以解吸的主要原因;基于H_2S气体在煤中吸附解吸特征,提出应从H_2S气体分子本身入手,结合矿井煤层地质条件来治理煤矿中的硫化氢。