CO2-CH4流体与金成矿作用:以阿尔泰山南缘和穆龙套金矿为例

造山型金矿的成矿作用与 H_2O-CO_2流体有着密切的联系。然而对阿尔泰山南缘和穆龙套金矿的流体包裹体研究表明,无水的 CO_2-CH_4流体在中亚成矿域中一些金矿床中具有同样重要意义。阿尔泰山南缘萨热阔布金矿包裹体的 X_(CH_4)达0.20～0.23,穆龙套金矿的 X_(CH_4)为0.07～0.23。CH_4扩大了流体不混溶的范围,有利于对 Au 的富集沉淀。CO_2流体在 Au 成矿中的重要作用至少包括了三方面的意义,即:缓冲流体 pH 值范围、提高流体中的 Au 含量并使其维持与还原硫的络合作用进行迁移;扩大超临界流体的温度范围;增加流体不混溶的区域。CH_4的加入扩大了流体不混溶的范围,有利于对 Au 的富集沉淀。     

黔西南灰家堡金矿田成矿流体来源及演化:流体包裹体和稳定同位素证据

为厘清滇黔桂地区卡林型金矿床成矿流体的特征,本文以灰家堡金矿田为代表,对太平洞、紫木凼、水银洞和簸箕田4个典型矿床中热液矿物的流体包裹体进行了系统研究,并对热液矿物进行了碳、氢、氧、硫同位素的分析测试。结果表明,灰家堡金矿田流体包裹体类型丰富,包括NaCl-H2O溶液包裹体、CO2包裹体、CO2-H2O包裹体、烃-H2O包裹体和烃类包裹体五大类。从成矿早阶段到晚阶段,成矿流体组分大致经历了从H2O+NaCl→H2O+NaCl+CO2+CH4±N2→H2O+NaCl±CH4±CO2的演化,均一温度和盐度略有降低。流体包裹体及稳定同位素组成特征显示,成矿流体属于富含金属和碳氢化合物的盆地流体;沉积黄铁矿的硫主要来源于封闭海洋盆地中硫酸盐的细菌还原硫;热液硫化物与沉积黄铁矿的硫同位素特征相似,表明成矿流体中的硫来源于成岩黄铁矿的溶解作用,同时有机质热分解和硫酸盐有机质热还原作用亦提供了部分硫。成矿主阶段发生的H2O-NaCl-CO2流体不混溶作用是导致Au沉淀富集的重要机制。     

黔西南紫木凼金矿床流体包裹体特征及对成矿的指示意义

紫木凼金矿床是黔西南微细浸染型（卡林型）金矿带上的一个代表性金矿床。本文对该矿床主成矿阶段（Ⅱ）石英和方解石以及晚成矿阶段（Ⅲ）方解石中的流体包裹体进行了岩相学和显微测温研究,结果表明,各成矿阶段包裹体类型有H2O包裹体、CO2包裹体、CO2-H2O包裹体、气相CH4包裹体和CH4-H2O包裹体5类,其中CO2包裹体和CO2-H2O包裹体只在主成矿阶段（Ⅱ）的石英中发育。主成矿阶段和晚阶段流体包裹体均一温度范围分别为180～220℃和100～180℃,盐度分别为0.35%～7.45% NaCl和0.18%～5.71% NaCl,密度分别变化于0.745～0.969 g/cm3和0.868～0.993 g/cm3,总体属于中低温、低盐度、中等密度的H2O-NaCl-CO2流体体系。矿床成矿过程是一个温度退缩、盐度降低、密度增大的过程。主成矿阶段H2O-NaCl-CO2流体发生不混溶作用,是导致矿质沉淀成矿的主要原因。CO2流体、CH4流体在金的成矿过程中起重要作用。     

河南祁雨沟金矿床成矿流体演化特征

祁雨沟隐爆角砾岩金矿床产于太古宇太华群中,金矿化分为6个成矿阶段,其中第Ⅰ,Ⅲ,Ⅴ阶段石英39Ar 40Ar坪年龄分别为130 31±0 86,122 61±0 61和(109 20±0 70)Ma。对各成矿阶段石英、方解石中流体包裹体均一温度、盐度、化学成分、氢氧同位素组成分析结果表明,早阶段流体为岩浆水,其后逐渐有大气降水的混合;第Ⅰ阶段高温(301 2～465 4℃)、中等盐度(9 1%～18 6%)的流体曾发生沸腾,形成较多以气相为主的包裹体;从第Ⅱ成矿阶段开始,流体沸腾减弱而出现不混溶现象;在第Ⅲ成矿阶段,不混溶作用增强,形成富CO2的低盐度流体与富H2O高盐度流体;在第Ⅳ—Ⅴ成矿阶段,大气降水的混合作用趋于增强,流体总体盐度降低。流体包裹体气相成分以CO2,H2S,CH4为主,含少量CO,N2,H2等,并且早阶段流体CO2含量较高,在第Ⅲ—Ⅴ成矿阶段,H2S,CH4,CO浓度增高,金属矿物大量出现。减压作用造成初始高温流体沸腾,其后温度降低以及盐析效应可能造成富CO2流体与富H2O流体的不混溶,而Au的大量沉淀则主要与大气降水的混合作用有关。     

澳大利亚纳沃日金矿流体混合与金的成矿作用

流体包裹体研究表明，纳沃日金矿成矿脉体中流体包裹体类型有三种，富CH4、CH4－CO2－H2O和富H2O包裹体。初始成矿流体是富CH4热液，在主矿化阶段，另一来源的CO2－H2O流体与CH4流体发生了不均匀混合，并且在石英－磁黄铁矿阶段最为强烈，造成不同矿化部位的xCH4变化极大，早期近于纯CH4流体被充分“稀释”后，石英－黄铁矿阶段的xCH4显著减小，到成矿晚期只剩CO2－H2O流体。正是由于不同性质流体的混合，造成热液的pH及fo2的升高，流体中的金－硫络合物分解，金沉淀成矿。     

CO2流体与金矿化：流体包裹体的证据

在世界的各种类型的金矿包括石英脉型、网脉型以及蚀变岩型金矿床中均见到H2O.CO2:和富含CO2的包裹体.在金矿的围岩蚀变中见到碳酸盐化、黄铁矿化、绢云母化和硅化,说明Au的成矿流体中有C2O和硫等这些组分.金矿床中的C2O流体包裹体有以下特点:(1)在金矿床中常见四类包裹体即水溶液包裹体、H2O-CO2包裹体、富CO2包裹体和含NaC1子矿物包裹体,但以前三者为主,这四类包裹体可以在一起分布,常见水溶液包裹体和CO2包裹体分别分开分布,常单独成行分布,显示出成矿流体的相分离.(2)CO2包裹体与自然金的关系,可以见到自然金与富CO2包裹体分布在同一行上,或者CO2流体与自然金产在一起,或者自然金分布于CO2包裹体中,说明Au是与CO2同时搬运和沉淀的.(3)对金矿中的流体包裹体成分分析表明,除Au、H2O和CO2是流体的主要成分外,还有少量的CH4、H2S和N2等.H2S和H2CO3的相图研究表明,Au的络合物可能是AuHS或AuH2S,这种Au的络合物只有在CO2作为缓冲剂的热液中其溶解度最大,这样的热液就是Au的成矿流体.这种流体在上升过程中与围岩发生交代作用形成蚀变,并且流体发生了相分离,分出相对富含H2O的流体和相对富含CO2的流体,Au在这种相分离的过程中与CO2一起沉淀下来,形成金矿.     

黑龙江省马连金矿床流体包裹体特征及其地质意义

为确定马连金矿成矿流体性质,笔者对成矿期石英开展详细的流体包裹体和氢氧同位素研究,包裹体岩相学和显微测温结果表明:石英中主要发育气相包裹体、液相包裹体和纯液相包裹体;包裹体均一温度为148~255℃(峰值为180~210℃),盐度为1.7%~7.5%Na Cleqv(峰值2%~4%Na Cleqv),属于低温、低盐度金矿床。激光拉曼和群体包裹体成分分析显示:成矿流体气相成分以H2O为主,CO2、CH4次之,液体主要成分为Ca2+、Na+、SO42-和F-,其次为K+、Mg2+、NO3-和Cl-,成矿流体属于Na Cl-H2O±CO2±CH4体系。包裹体氢氧同位素研究表明:成矿流体δDV-SMOW值介于-92.3‰~-113.4‰,δ18OH2O值介于2.5‰~3.5‰,具有岩浆水和大气降水混合的特征,结合成矿流体特征,认为流体不混溶或沸腾作用导致相分离是马连金矿沉淀主要原因。     

阿勒泰恰夏铜矿床的富CO2流体与矿床成因

恰夏铜矿床位于新疆阿尔泰山南缘克兰火山-沉积盆地内,赋矿地层主要为下泥盆统康布铁堡组上亚组变质岩系.脉状铜矿化主要特征为:早期顺层石英脉,呈脉状或透镜状沿变质片理分布,有星点状黄铁矿产出;晚期含铜黄铁矿-石英脉,斜切变质围岩,黄铜矿以浸染状分布于石英脉裂隙中.石英脉中流体包裹体主要为富CO2包裹体,其次为水溶液包裹体,同时含有少量的碳质流体包裹体.显微测温研究表明,早期顺层石英中原生富CO2流体包裹体,CO2三相点温度(tm,CO2)集中在-61.5～-57.5℃,CO2部分均一温度(th,CO2)集中在25～27℃,完全均一温度(th,tot)集中于223～280℃,流体密度为0.82～0.90 g/cm3;含铜黄铁矿-石英脉中原生富CO2包裹体的tm,CO2集中于-61.5～-58.7℃,th,CO2集中在23.5～28.7℃,th,tot集中在230 ～ 310℃,流体密度0.81～0.86 g/cm3.成矿流体为中高温、中低盐度、富CO2的CO2-H2O-NaCl±CH4±N2体系.恰夏铜矿脉状铜矿化的成矿流体特征与造山型金矿床的流体包裹体特征类似,结合矿床产出的地质背景、控矿构造特征,认为脉状铜矿化的成因与造山-变质热液有关,是阿尔泰山南缘晚泥盆世一二叠纪造山-变质作用的产物.SRXRF测试富CO2流体包裹体中金属微量元素,显示其富集Au,可能表明富CO2流体对金的富集起到一定作用.     

新疆萨瓦亚尔顿金矿流体包裹体成分、矿床成因和成矿预测

新疆萨瓦亚尔顿金矿区发育含矿和无矿石英脉,无矿石英、含矿石英及主要载金矿物黄铁矿所含包裹体捕获的流体成分有明显差异,分别代表了成矿前、成矿早阶段和主成矿阶段的流体特征。早阶段成矿物质沉淀的主要机制为流体不混溶作用,形成含矿石英、含钠矿物和部分黄铁矿等;主成矿阶段则以流体浓缩及流体混合为主要机制,形成大量黄铁矿等载金矿物。萨瓦亚尔顿金矿的成矿流体成分特征与世界造山型的中温热液脉状金矿类似,尤其是与乌兹别克南天山造山带的穆龙套金矿类似,表明其为较典型的穆龙套式的造山型金矿床。Ⅺ、Ⅱ矿化带流体成分特征与矿化最好的Ⅳ带类似,勘探前景较好;相反,Ⅰ矿化带与Ⅳ带差异明显,不宜作为勘探重点。     

北山金窝子金矿床流体包裹体特征及成矿流体演化

金窝子金矿床为于甘肃北山中成矿带。包裹体测温研究表明，从成矿初期到主成矿阶段，石英捕获了H2O—NaCl，H2O-CO2-CH4-NaCl，或H2O-CO2-NaCl体系的流体。大脉型金矿成矿初期，热液成矿流体由高温中盐度H2O-NaCl-CO2-CH4四端元组份混溶的均一相热液流体；石英-黄铁矿和多金属硫化物阶段，石英捕获两成分和温度都不相同的热液组份：低盐度、富水溶液、较冷的热液和高盐度、富挥发份CO2、CH4和水蒸气、较热的热液。主成矿阶段石英捕获的两类型包裹体的完全均一温度相差近100℃，而且富挥发份流体盐度相对于贫挥发份流体盐度高，上述特征表明主成矿期3号脉大规模金成矿并非流体沸腾作用结果。网脉型金矿（210号脉）黄铁矿-石英成矿阶段、石英．黄铁矿和多金属硫化物成矿阶段石英捕获的地质流体的温度-成分特征无明显差异，均捕获了两种组份不同、成矿温度一 致的地质流体（高盐度富水溶液流体和富堤盐度CO2＋CH4流体），与许多金矿的流体不混溶金成矿机制矛盾。     

Thermochemistry of glasses and liquids in the systems CaMgSi2O6-CaAl2Si2O8-NaAlSi3O8, SiO2-CaAl2Si2O8-NaAlSi3O8 and SiO2-Al2O3-CaO-Na2O

Enthalpies of solution in 2PbO· B₂O₃ at 712°C have been measured for glasses in the systems albite anorthite diopside, NaAlO₂-SiO₂, Ca_0.5AlO₂-SiO₂ and albite-anorthite-quartz. The systems albite-anorthite and diopside-anorthite show substantial negative enthalpies of mixing, albite-diopside shows significant positive heats of mixing. For compositions up to NaAlO₂ = 0.42 (which includes the subsystem albite-silica) the system NaAlO₂-SiO₂ shows essentially zero heats of mixing. A negative ternary excess heat of mixing is found in the plagioclase-rich portion of the albite-anorthite-diopside system. The join Si₄O₈-CaAl₂Si₂O₈ shows small but significant heats of mixing. In albite-anorthite-quartz. ternary glasses, the ternary excess enthalpy of mixing is positive.Based on available heat capacity data and appropriate consideration of the glass transition, the enthalpy of the crystal-glass transition (vitrification) is a serious underestimate of the enthalpy of the crystal-liquid transition (fusion) especially when the melting point, T_f, is many hundreds of degrees higher than the glass transition temperature, T_g. On the other hand, the same heat capacity data suggest that the enthalpies of mixing in albite-anorthite-diopside liquids are calculated to be quite similar to those in the glasses. The enthalpies of mixing observed in general support the structural models proposed by Taylor and Brown (1979a, b) and others for the structure of aluminosilicate glasses.     

Thermochemical study of glasses in the system NaAlSi3O8-KAlSi3O8-Si4O8 and the join Na1.6Al1.6Si2.4O8-K1.6Al1.6Si2.4O8

Enthalpies of solution in 2PbO · B₂O₃ at 981 K have been measured for glasses in the system albite-orthoclase-silica and along the join Na_1.6Al_1.6Si_2.4O₈-K_1.6Al_1.6Si_2.4O₈. The join KAlSi₃O₈-Si₄O₈ shows zero heat of mixing similar to that found previously for NaAlSi₃O₈-Si₄O₈ glasses. Albite-orthoclase glasses show negative heats of mixing symmetric about Ab₅₀Or₅₀ (W_n = ? 2.4 ± 0.8 kcal). Negative heats of (Na, K) mixing are also found at $\text{Si}\text{(Si + Al)}\text{= 0.6.}$ Ternary excess enthalpies of mixing in the glassy system Ab-Or-4Q are positive but rarely exceed 1 kcal mol^?1.Using earlier studies of the thermodynamic properties of the crystals, the present calorimetric data and the “two-lattice” entropy model, the albite-orthoclase phase diagram is calculated in good agreement with experimental data. Attempts to calculate albite-silica and orthoclase-silica phase diagrams reveal complexities probably related to significant (but unknown) mutual solid solubility between cristobalite and alkali feldspar and to the very small heat and entropy of fusion of SiO₂.     

A hydrofluoric acid solution calorimetric investigation of glasses in the systems NaAlSi3O8-KAlSi3O8 and NaAlSi3O8-Si4O8

Glasses in the systems NaAlSi₃O₈-KAlSi₃O₈ and NaAlSi₃O₈-Si₄O₈ have been studied by means of hydrofluoric acid solution calorimetry at 50°C. Results indicate small negative enthalpies of mixing in the former system and small positive departures from ideality in the latter.     

The MgO-Al2O3-SiO2 system: free energy of pyrope and Al2O3-enstatite

Using the model of fictive ideal components, Gibbs free energies of formation of pyrope and Al₂O₃-enstatite have been determined from the experimental data on coexisting garnet and orthopyroxene and orthopyroxene and spinel in the temperature range of 1200–1600 K. The negative free energies in kJ/mol are:

     

15.

Thermochemistry of glasses along joins of pyroxene stoichiometry in the system Ca₂Si₂O₆-Mg₂Si₂O₆-Al₄O₆     

Richard L. Hervig  Derry Scott  Alexandra Navrotsky 《Geochimica et cosmochimica acta》1985,49(7):1497-1501

Enthalpies of solution in 2PbO · B₂O₃ at 974 K have been measured for glasses along the joins Ca₂Si₂O₆ (Wo)-Mg₂Si₂O₆ (En) and Mg₂Si₂O₆-MgAl₂SiO₆ (MgTs). Heats of mixing are symmetric and negative for Wo-En with W_H = ?31.0 ± 3.6 kJ mol^?. Negative heats of mixing were also found for the En-MgTs glasses (W_H = ?33.4 ± 3.7 kJ mol^?).Enthalpies of vitrification of pyroxenes and pyroxenoids generally increase with decreasing alumina content and with decreasing basicity of the divalent cation.Heats of mixing along several glassy joins show systematic trends. When only non-tetrahedral cations mix (outside the aluminosilicate framework), small exothermic heats of mixing are seen. When both nontetrahedral and framework cations mix (on separate sublattices, presumably), the enthalpies of mixing are substantially more negative. Maximum enthalpy stabilization near compositions with Al/Si ≈ 1 is suggested.     

16.

Polymerization of silicate and aluminate tetrahedra in glasses,melts, and aqueous solutions—I. Electronic structure of H₆Si₂O₇, H₆AlSiO₇¹⁻, and H₆Al₂O₇²⁻     

B.H.W.S. de Jong  Gordon E. Brown 《Geochimica et cosmochimica acta》1980,44(3):491-511

As part of a study of the effect of geologically common network modifiers on polymerization in silicate melts, glasses, and silica-rich aqueous solutions, we have studied the energies, electronic structures, and inferred chemical properties of ^IVT-O-^IVT linkages in the tetrahedral dimers H₆,Si₂O₇, H₆AlSiO₇^1?, and H₆Al₂O₇^2? using semi-empirical molecular orbital theory (CNDO/2). Our results indicate that the electron donating character of the bridging oxygen, O(br), linking two tetrahedra increases with increasing T-O(br) bond length but decreases with decreasing T-O(br)-T angles and increasing O-T-O(br) angles. This increase or decrease of the donor character of O(br) coincides with an increase or decrease of the affinity of O(br) for hard acceptors. The calculated electronic structure for the H₆Si₂O₇ molecule is compared with the observed X-ray emission, absorption, and photoelectron spectra of quartz and vitreous silica; the reasonable match between calculated and observed oxygen Kα emission spectra of vitreous silica supports our assertion that non-bonded O(br) electron density energetically at the top of the valence band controls the chemical reactivity of ^IVT-O-^IVT linkages in polymerized tetrahedral environments.     

17.

Molecular H₂O in armenite, BaCa₂Al₆Si₉O₃₀·2H₂O, and epididymite, Na₂Be₂Si₆O₁₅·H₂O: Heat capacity, entropy and local-bonding behavior of confined H₂O in microporous silicates     

Charles A. Geiger  Edgar Dachs  Gilberto Artioli 《Geochimica et cosmochimica acta》2010,74(18):5202-5215

Armenite, ideal formula BaCa₂Al₆Si₉O₃₀·2H₂O, and its dehydrated analog BaCa₂Al₆Si₉O₃₀ and epididymite, ideal formula Na₂Be₂Si₆O₁₅·H₂O, and its dehydrated analog Na₂Be₂Si₆O₁₅ were studied by low-temperature relaxation calorimetry between 5 and 300 K to determine the heat capacity, C_p, behavior of their confined H₂O. Differential thermal analysis and thermogravimetry measurements, FTIR spectroscopy, electron microprobe analysis and powder Rietveld refinements were undertaken to characterize the phases and the local environment around the H₂O molecule.The determined structural formula for armenite is Ba_0.88(0.01)Ca_1.99(0.02)Na_0.04(0.01)Al_5.89(0.03)Si_9.12(0.02)O₃₀·2H₂O and for epididymite Na_1.88(0.03)K_0.05(0.004)Na_0.01(0.004)Be_2.02(0.008)Si_6.00(0.01)O₁₅·H₂O. The infrared (IR) spectra give information on the nature of the H₂O molecules in the natural phases via their H₂O stretching and bending vibrations, which in the case of epididymite only could be assigned. The powder X-ray diffraction data show that armenite and its dehydrated analog have similar structures, whereas in the case of epididymite there are structural differences between the natural and dehydrated phases. This is also reflected in the lattice IR mode behavior, as observed for the natural phases and the H₂O-free phases. The standard entropy at 298 K for armenite is S° = 795.7 ± 6.2 J/mol K and its dehydrated analog is S° = 737.0 ± 6.2 J/mol K. For epididymite S° = 425.7 ± 4.1 J/mol K was obtained and its dehydrated analog has S° = 372.5 ± 5.0 J/mol K. The heat capacity and entropy of dehydration at 298 K are Δ = 3.4 J/mol K and ΔS^rxn = 319.1 J/mol K and Δ = −14.3 J/mol K and ΔS^rxn = 135.7 J/mol K for armenite and epididymite, respectively. The H₂O molecules in both phases appear to be ordered. They are held in place via an ion-dipole interaction between the H₂O molecule and a Ca cation in the case of armenite and a Na cation in epididymite and through hydrogen-bonding between the H₂O molecule and oxygen atoms of the respective silicate frameworks. Of the three different H₂O phases ice, liquid water and steam, the C_p behavior of confined H₂O in both armenite and epididymite is most similar to that of ice, but there are differences between the two silicates and from the C_p behavior of ice. Hydrogen-bonding behavior and its relation to the entropy of confined H₂O at 298 K is analyzed for various microporous silicates.The entropy of confined H₂O at 298 K in various silicates increases approximately linearly with increasing average wavenumber of the OH-stretching vibrations. The interpretation is that decreased hydrogen-bonding strength between a H₂O molecule and the silicate framework, as well as weak ion-dipole interactions, results in increased entropy of H₂O. This results in increased amplitudes of external H₂O vibrations, especially translations of the molecule, and they contribute strongly to the entropy of confined H₂O at T < 298 K.     

18.

Alkali-free tourmaline in the system MgO-Al₂O₃-B₂O₃-SiO₂-H₂O     

Günter Werding  Werner Schreyer 《Geochimica et cosmochimica acta》1984,48(6):1331-1344

An end member of the tourmaline series with a structural formula □(Mg₂Al)Al₆(BO₃)₃[Si₆O₁₈](OH)₄ has been synthesized in the system MgO-Al₂O₃-B₂O₃-SiO₂-H₂O where it represents the only phase with a tourmaline structure. Our experiments provide no evidence for the substitutions Al → Mg + H, Mg → 2H, B + H → Si, and AlAl → MgSi and we were not able to synthesize a phase “Mg-aluminobuergerite” characterized by Mg in the (3a)-site and a strong (OH)-deficiency reported by Rosenberg and Foit (1975). The alkali-free tourmaline has a vacant (3a)-site and is related to dravite by the □ + Al for Na + Mg substitution. It is stable from at least 300°C to about 800°C at low fluid pressures and 100% excess B₂O₃, and can be synthesized up to a pressure of 20 kbars. At higher temperatures the tourmaline decomposes into grandidierite or a boron-bearing phase possibly related to mullite (“B-mullite”), quartz, and unidentified solid phases, or the tourmaline melts incongruently into corundum + liquid, depending on pressure. In the absence of excess B₂O₃ tourmaline stability is lowered by about 60°C. Tourmaline may coexist with the other MgO-Al₂O₃-B₂O₃-SiO₂-H₂O phases forsterite, enstatite, chlorite, talc, quartz, grandidierite, corundum, spinel, “B-mullite,” cordierite, and sinhalite depending on the prevailing PTX-conditions.The (3a)-vacant tourmaline has the space group R3m with $\text{a =15.90}\text{A}\text{?}$, $\text{c = 7.115}\text{A}\text{?}$, and $\text{V = 1557.0}\text{A}\text{?}{}^3$. However, these values vary at room temperature with the pressure-temperature conditions of synthesis by $\text{±0.015}\text{A}\text{?}\text{in a}$, $\text{±0.010}\text{A}\text{?}\text{in c}$, and $\text{±4.0}\text{A}\text{?}{}^3\text{in V}$, probably as a result of MgAl order/disorder relations in the octahedral positions. Despite these variations intensity calculations support the assumed structural formula. Refractive indices are n_o = 1.631(2), n_E = 1.610(2), Δn = 0.021. The infrared spectrum is intermediate between those of dravite and elbaite. The common alkali and calcium deficiencies of natural tourmalines may at least partly be explained by miscibilities towards (3a)-vacant end members. The apparent absence of (3a)-vacant tourmaline in nature is probably due to the lack of fluids that carry boron but no Na or Ca.     

19.

N₂-CH₄（CO₂）混合气体在线标样制备及其拉曼定量因子测定   总被引：1，自引：1，他引：0  

席斌斌  施伟军  蒋宏  钱一雄 《岩矿测试》2014,33(5):655-660

利用混合气体的标准样品对激光拉曼探针进行标定,可以快速准确地对包裹体中的无机及有机气相组分进行定量分析。而常用的商用钢瓶装混合气体标样,存在费用高、气体组成单一固定等缺点。本文设计了一套在线标样制备装置,提出一种在线配置不同浓度和压力条件下混合气体标样的方法。利用高纯度(纯度99.999%)的N2、CH4以及CO2钢瓶气,经过在线混合增压,在5 MPa和10 MPa条件下制备了N2摩尔分数为30%、50%和70%的N2-CH4以及N2-CO2混合气体在线标样。该方法制备的标样与70%N2+30%CO2的商用钢瓶气标样对比表明,CO2与N2的拉曼相对峰高以及相对峰面积值的误差在4%以内,具有较高的准确度和重现性。通过不同压力和浓度条件下CH4以及CO2的拉曼相对定量因子测定表明,气体的相对定量因子在5~10 MPa压力条件下与压力及组成无关。地质样品应用结果表明,本方法可以方便、灵活、准确地按任意比例将两瓶及两瓶以上纯气体钢瓶样品进行混合及增压,为激光拉曼标定、气体组成原位测量等提供了一种新的技术思路。     

20.

Experimental study of the Mg₃Al₂Si₃O₁₂-Na₂MgSi₅O₁₂ system at 7.0 and 8.5 GPa: Implication for the formation of Na-bearing garnets     

A. V. Bobrov  Yu. A. Litvin 《Doklady Earth Sciences》2008,419(2):339-343

     

TK	1200	1300	1400	1500	1600
Pyrope	4869.92	4747.05	4614.26	4462.63	4311.00
Al2O3-enstatite	1257.25	1244.28	1191.93	1158.67	1125.64

Thermochemistry of glasses along joins of pyroxene stoichiometry in the system Ca2Si2O6-Mg2Si2O6-Al4O6

Enthalpies of solution in 2PbO · B₂O₃ at 974 K have been measured for glasses along the joins Ca₂Si₂O₆ (Wo)-Mg₂Si₂O₆ (En) and Mg₂Si₂O₆-MgAl₂SiO₆ (MgTs). Heats of mixing are symmetric and negative for Wo-En with W_H = ?31.0 ± 3.6 kJ mol^?. Negative heats of mixing were also found for the En-MgTs glasses (W_H = ?33.4 ± 3.7 kJ mol^?).Enthalpies of vitrification of pyroxenes and pyroxenoids generally increase with decreasing alumina content and with decreasing basicity of the divalent cation.Heats of mixing along several glassy joins show systematic trends. When only non-tetrahedral cations mix (outside the aluminosilicate framework), small exothermic heats of mixing are seen. When both nontetrahedral and framework cations mix (on separate sublattices, presumably), the enthalpies of mixing are substantially more negative. Maximum enthalpy stabilization near compositions with Al/Si ≈ 1 is suggested.     

Polymerization of silicate and aluminate tetrahedra in glasses,melts, and aqueous solutions—I. Electronic structure of H6Si2O7, H6AlSiO71−, and H6Al2O72−

As part of a study of the effect of geologically common network modifiers on polymerization in silicate melts, glasses, and silica-rich aqueous solutions, we have studied the energies, electronic structures, and inferred chemical properties of ^IVT-O-^IVT linkages in the tetrahedral dimers H₆,Si₂O₇, H₆AlSiO₇^1?, and H₆Al₂O₇^2? using semi-empirical molecular orbital theory (CNDO/2). Our results indicate that the electron donating character of the bridging oxygen, O(br), linking two tetrahedra increases with increasing T-O(br) bond length but decreases with decreasing T-O(br)-T angles and increasing O-T-O(br) angles. This increase or decrease of the donor character of O(br) coincides with an increase or decrease of the affinity of O(br) for hard acceptors. The calculated electronic structure for the H₆Si₂O₇ molecule is compared with the observed X-ray emission, absorption, and photoelectron spectra of quartz and vitreous silica; the reasonable match between calculated and observed oxygen Kα emission spectra of vitreous silica supports our assertion that non-bonded O(br) electron density energetically at the top of the valence band controls the chemical reactivity of ^IVT-O-^IVT linkages in polymerized tetrahedral environments.     

Molecular H2O in armenite, BaCa2Al6Si9O30·2H2O, and epididymite, Na2Be2Si6O15·H2O: Heat capacity, entropy and local-bonding behavior of confined H2O in microporous silicates

Armenite, ideal formula BaCa₂Al₆Si₉O₃₀·2H₂O, and its dehydrated analog BaCa₂Al₆Si₉O₃₀ and epididymite, ideal formula Na₂Be₂Si₆O₁₅·H₂O, and its dehydrated analog Na₂Be₂Si₆O₁₅ were studied by low-temperature relaxation calorimetry between 5 and 300 K to determine the heat capacity, C_p, behavior of their confined H₂O. Differential thermal analysis and thermogravimetry measurements, FTIR spectroscopy, electron microprobe analysis and powder Rietveld refinements were undertaken to characterize the phases and the local environment around the H₂O molecule.The determined structural formula for armenite is Ba_0.88(0.01)Ca_1.99(0.02)Na_0.04(0.01)Al_5.89(0.03)Si_9.12(0.02)O₃₀·2H₂O and for epididymite Na_1.88(0.03)K_0.05(0.004)Na_0.01(0.004)Be_2.02(0.008)Si_6.00(0.01)O₁₅·H₂O. The infrared (IR) spectra give information on the nature of the H₂O molecules in the natural phases via their H₂O stretching and bending vibrations, which in the case of epididymite only could be assigned. The powder X-ray diffraction data show that armenite and its dehydrated analog have similar structures, whereas in the case of epididymite there are structural differences between the natural and dehydrated phases. This is also reflected in the lattice IR mode behavior, as observed for the natural phases and the H₂O-free phases. The standard entropy at 298 K for armenite is S° = 795.7 ± 6.2 J/mol K and its dehydrated analog is S° = 737.0 ± 6.2 J/mol K. For epididymite S° = 425.7 ± 4.1 J/mol K was obtained and its dehydrated analog has S° = 372.5 ± 5.0 J/mol K. The heat capacity and entropy of dehydration at 298 K are Δ = 3.4 J/mol K and ΔS^rxn = 319.1 J/mol K and Δ = −14.3 J/mol K and ΔS^rxn = 135.7 J/mol K for armenite and epididymite, respectively. The H₂O molecules in both phases appear to be ordered. They are held in place via an ion-dipole interaction between the H₂O molecule and a Ca cation in the case of armenite and a Na cation in epididymite and through hydrogen-bonding between the H₂O molecule and oxygen atoms of the respective silicate frameworks. Of the three different H₂O phases ice, liquid water and steam, the C_p behavior of confined H₂O in both armenite and epididymite is most similar to that of ice, but there are differences between the two silicates and from the C_p behavior of ice. Hydrogen-bonding behavior and its relation to the entropy of confined H₂O at 298 K is analyzed for various microporous silicates.The entropy of confined H₂O at 298 K in various silicates increases approximately linearly with increasing average wavenumber of the OH-stretching vibrations. The interpretation is that decreased hydrogen-bonding strength between a H₂O molecule and the silicate framework, as well as weak ion-dipole interactions, results in increased entropy of H₂O. This results in increased amplitudes of external H₂O vibrations, especially translations of the molecule, and they contribute strongly to the entropy of confined H₂O at T < 298 K.     

Alkali-free tourmaline in the system MgO-Al2O3-B2O3-SiO2-H2O

An end member of the tourmaline series with a structural formula □(Mg₂Al)Al₆(BO₃)₃[Si₆O₁₈](OH)₄ has been synthesized in the system MgO-Al₂O₃-B₂O₃-SiO₂-H₂O where it represents the only phase with a tourmaline structure. Our experiments provide no evidence for the substitutions Al → Mg + H, Mg → 2H, B + H → Si, and AlAl → MgSi and we were not able to synthesize a phase “Mg-aluminobuergerite” characterized by Mg in the (3a)-site and a strong (OH)-deficiency reported by Rosenberg and Foit (1975). The alkali-free tourmaline has a vacant (3a)-site and is related to dravite by the □ + Al for Na + Mg substitution. It is stable from at least 300°C to about 800°C at low fluid pressures and 100% excess B₂O₃, and can be synthesized up to a pressure of 20 kbars. At higher temperatures the tourmaline decomposes into grandidierite or a boron-bearing phase possibly related to mullite (“B-mullite”), quartz, and unidentified solid phases, or the tourmaline melts incongruently into corundum + liquid, depending on pressure. In the absence of excess B₂O₃ tourmaline stability is lowered by about 60°C. Tourmaline may coexist with the other MgO-Al₂O₃-B₂O₃-SiO₂-H₂O phases forsterite, enstatite, chlorite, talc, quartz, grandidierite, corundum, spinel, “B-mullite,” cordierite, and sinhalite depending on the prevailing PTX-conditions.The (3a)-vacant tourmaline has the space group R3m with $\text{a =15.90}\text{A}\text{?}$, $\text{c = 7.115}\text{A}\text{?}$, and $\text{V = 1557.0}\text{A}\text{?}{}^3$. However, these values vary at room temperature with the pressure-temperature conditions of synthesis by $\text{±0.015}\text{A}\text{?}\text{in a}$, $\text{±0.010}\text{A}\text{?}\text{in c}$, and $\text{±4.0}\text{A}\text{?}{}^3\text{in V}$, probably as a result of MgAl order/disorder relations in the octahedral positions. Despite these variations intensity calculations support the assumed structural formula. Refractive indices are n_o = 1.631(2), n_E = 1.610(2), Δn = 0.021. The infrared spectrum is intermediate between those of dravite and elbaite. The common alkali and calcium deficiencies of natural tourmalines may at least partly be explained by miscibilities towards (3a)-vacant end members. The apparent absence of (3a)-vacant tourmaline in nature is probably due to the lack of fluids that carry boron but no Na or Ca.     

N2-CH4（CO2）混合气体在线标样制备及其拉曼定量因子测定

利用混合气体的标准样品对激光拉曼探针进行标定,可以快速准确地对包裹体中的无机及有机气相组分进行定量分析。而常用的商用钢瓶装混合气体标样,存在费用高、气体组成单一固定等缺点。本文设计了一套在线标样制备装置,提出一种在线配置不同浓度和压力条件下混合气体标样的方法。利用高纯度(纯度99.999%)的N2、CH4以及CO2钢瓶气,经过在线混合增压,在5 MPa和10 MPa条件下制备了N2摩尔分数为30%、50%和70%的N2-CH4以及N2-CO2混合气体在线标样。该方法制备的标样与70%N2+30%CO2的商用钢瓶气标样对比表明,CO2与N2的拉曼相对峰高以及相对峰面积值的误差在4%以内,具有较高的准确度和重现性。通过不同压力和浓度条件下CH4以及CO2的拉曼相对定量因子测定表明,气体的相对定量因子在5~10 MPa压力条件下与压力及组成无关。地质样品应用结果表明,本方法可以方便、灵活、准确地按任意比例将两瓶及两瓶以上纯气体钢瓶样品进行混合及增压,为激光拉曼标定、气体组成原位测量等提供了一种新的技术思路。