西拉沐伦钼矿带车户沟斑岩型钼-铜矿床成矿流体特征及其地质意义   总被引：9，自引：4，他引：5  

褚少雄  曾庆栋  刘建明  张伟庆  张作伦  张松  汪在聪 《岩石学报》2010,26(8):2465-2481

车户沟钼-铜矿床是华北克拉通北缘西拉沐伦钼矿带上典型的斑岩型Mo-Cu矿床,位于华北克拉通北缘断裂南侧。矿床赋存于成矿母岩花岗斑岩及其围岩中,矿化类型以细脉浸染状矿化为主,还存在隐爆角砾岩型矿化和石英脉型矿化。根据脉体类型和矿物组合将车户沟钼-铜矿床划分为四个成矿阶段,分别为(1)辉钼矿-黄铁矿-石英阶段、(2)黄铜矿+黄铁矿±辉钼矿+石英阶段、(3)黄铁矿+石英阶段、(4)石英+碳酸盐±萤石阶段。成矿流体寄主矿物石英中发育Ⅰ型含CO2三相包裹体(LCO2+VCO2+LH2O)、Ⅱ型含子晶三相(V-L+S)包裹体、Ⅲ型富气相(V-L)包裹体、Ⅳ型富液相(L-V)包裹体、Ⅴ型纯气相(V)包裹体和Ⅵ型纯液相(L)六种类型。流体包裹体类型从早到晚具有规律性演化特征,表现为阶段(1)、(2)以发育Ⅰ型含CO2三相包裹体(LCO2+VCO2+LH2O)和Ⅱ型含子晶三相(V-L+S)包裹体为特征,成矿晚期阶段(3)、(4)以发育Ⅲ型富气相(V-L)包裹体、Ⅳ型富液相(L-V)水溶液包裹体为特征。从早阶段到晚阶段成矿流体温度及盐度具有规律性演化特征。均一温度峰值分别为270～400℃、230～370℃、160～290℃、120～230℃,成矿温度逐渐降低;流体盐度,阶段(1)流体盐度分两组:3.39%～14.25%NaCleqv和31.01%～66.75%NaCleqv、阶段(2)流体盐度分两组:1.23%～12.85%NaCleqv和31.14%～64.33%NaCleqv、阶段(3)、(4)盐度分别介于1.05%～21.47%NaCleqv和2.07%～10.73%NaCleqv,盐度逐渐降低。激光拉曼显微探针(LRM)及群体包裹体成分分析结果表明,流体体系成分以H2O、CO2、Cl-、SO42-、Na+为主,贫F-、Ca2+、Mg2+为特征,特征离子比值暗示流体来源于岩浆流体。包裹体岩相学及包裹体测温表明,流体由早期的高温、高盐度、含二氧化碳NaCl-H2O-CO2体系岩浆流体在主成矿阶段(1)、(2)发生流体包裹体的沸腾作用和相分离,伴随流体沸腾、CO2逸失、温度降低等过程导致大量金属硫化物沉淀。成矿晚期阶段(3)、(4),成矿体系趋于开放,流体存在大气降水混入演化为晚期中-低温、中-低盐度贫CO2的NaCl-H2O流体体系。成矿作用机制上沸腾作用是导致主成矿期辉钼矿、黄铜矿沉淀成矿的重要机制。成矿作用晚期阶段(3)、(4)流体混合作用成为成矿作用的主导机制。  相似文献   

长江中下游池州地区矽卡岩-斑岩型W-Mo矿床流体包裹体与H、O、S同位素研究   总被引：7，自引：5，他引：2  

宋国学  秦克章  李光明 《岩石学报》2010,26(9):2768-2782

长江中下游池州地区区域构造上处于下扬子坳陷与江南古陆之间的过渡带上,近年来该区域内以钨钼为主的多金属矿床勘探方面取得了很大突破,鸡头山矽卡岩-斑岩型W-Mo矿、马头斑岩型Mo矿和百丈岩矽卡岩-斑岩型W-Mo矿是其中的三个代表性矿床。在鸡头山矿区和百丈岩矿区钨钼主要赋存于矽卡岩体中,已有工程探明二者的深部都有斑岩型矿体存在;在马头矿区钼主要以含钼石英脉和辉钼矿细脉的形式赋存于近接触带岩体与围岩中。流体包裹体研究表明,池州地区与钨钼矿有关的流体包裹体以水溶液包裹体(L+V)为主,同时发育含子矿物包裹体(L+V+S)和CO2包裹体(L+LCO2+VCO2)。成矿流体演化分为三个阶段:早阶段温度在350～500℃之间,深度约为1.5～2.5km,初始流体盐度为17%～25%NaCleqv,流体富H2O-CO2-CH4等气体,流体发生沸腾作用分离出高盐度流体和富气相低盐度流体;中阶段温度在170～360℃之间,深度约为0.5～1.7km,盐度为2%～24%NaCleqv,富H2O-CO2-CH4-H2S等气体,流体混合作用使得大量钨、钼、铅、锌等金属沉淀成矿;晚阶段温度在100～160℃之间,深度在约0.6km以下,盐度范围为1%～10%NaCleqv,与成矿作用无关。含矿石英脉H-O同位素和硫化物S同位素共同指示,池州地区与钨钼矿有关的成矿流体来自岩浆水、大气水和建造水的混合,流体混合是区域钨-钼-铅-锌成矿的主要机制。  相似文献   

构造应力环境对浅成岩体成矿系统的制约:从安庆月山岩体冷却过程动力学计算模拟结果分析   总被引：2，自引：0，他引：2  

刘亮明  周瑞超  赵崇斌 《岩石学报》2010,26(9):2869-2878

为探讨构造应力环境对浅成岩体成矿系统的制约,以安庆地区的月山岩体及其所形成的安庆铜矿床为例,在传统地质调查研究的基础上,通过假设不同的力学边界条件进行岩体冷却过程动力学的计算模拟实验研究。计算结果显示,在没有构造应力作用时,在岩体的接触带上不可能形成有利成矿定位的局部汇流扩容空间,挤压和拉伸作用都能够在岩体接触带形成局部汇流扩容空间,但二者的空间分布规律有着极大的差别,只有拉伸构造应力作用下的动力学计算模拟实验能在已发现矿体部位形成汇流扩容空间,表明构造应力环境对成矿定位的汇流空间的制约以及拉伸构造应力作用对月山岩体成矿的重要贡献。在拉伸构造应力和无构造应力作用时,接触带上的流体压力都是随着变形的进程而趋降低的,只有在挤压构造应力作用下,流体压力才会有一个超压的过程,流体超压是形成斑岩型矿床的重要机制。可见挤压环境才是一种有利于斑岩型矿床成矿的构造环境,铜陵-安庆地区缺乏与矽卡岩矿床相对应的斑岩型矿床主要原因之一是成矿时处于一种拉伸的构造应力作用环境。  相似文献   

山东金岭金矿床成矿流体地球化学特征   总被引：4，自引：0，他引：4  

王力  孙丰月  王佳良 《岩石学报》2010,26(12):3735-3744

对山东金岭金矿矿石中的流体包裹体进行了岩相学、显微测温及单个包裹体成分激光拉曼光谱研究。结果表明:金矿石中发育含CO2相、气液两相和CO2相等三类包裹体,成矿过程中,流体经历了NaCl-H2O-CO2体系的不混溶作用;成矿流体具有低盐度(6.6%~10.8%NaCleqv)、低密度(0.54~0.93g.cm-3)的特点;成矿温度集中于280~300℃之间,成矿压力为70~119MPa,成矿深度为6.78~9.07km;矿石石英中流体包裹体成分普遍含CO2。结合新近的流体包裹体同位素分析结果和测年数据,认为成矿流体为地幔流体、岩浆流体和大气降水的混合产物,矿床成因类型为幔源流体参与成矿的造山型金矿床中成亚类。  相似文献   

Mud volcanism and fluid geochemistry in the Cheleken peninsula,western Turkmenistan     

《Marine and Petroleum Geology》2014

A geological and geochemical study has been carried out to investigate the relationships between major mud volcano structures and deep fluid migration in the Cheleken peninsula, in the South Caspian Basin. The fluid geochemistry allowed the origin and migration of the saline waters and the hydrocarbons to be deduced along with the regional source and reservoir rocks. The emitted waters formed by the mixing of deep highly saline water from the main source rocks of the Maykop Fm with the Caspian-like pore water contained in the Pliocene reservoirs. The water composition is very similar to that emitted by the mud volcanoes in Azerbaijan, allowing comparisons to be done between the reservoirs in the western and eastern sides of the South Caspian Basin. The associated oil is derived from a mixed type II/III kerogen deposited in a sub-oxic marine environment and generated during the early oil window. The oil biomarkers indicate that the source rock is the Maykop Fm., as previously determined for the other areas of the South Caspian Basin.The spontaneous emissions, showing different morphologies, are mainly aligned along normal and transtensive fault systems, which provide effective pathways for rapid fluid ascent from deep reservoirs to the surface.  相似文献   

Geochronology and fluid inclusion study of the Yinjiagou porphyry–skarn Mo–Cu–pyrite deposit in the East Qinling orogenic belt,China     

《Journal of Asian Earth Sciences》2014

The Yinjiagou Mo–Cu–pyrite deposit of Henan Province is located in the Huaxiong block on the southern margin of the North China craton. It differs from other Mo deposits in the East Qingling area because of its large pyrite resource and complex associated elements. The deposit’s mineralization process can be divided into skarn, sulfide, and supergene episodes with five stages, marking formation of magnetite in the skarn episode, quartz–molybdenite, quartz–calcite–pyrite–chalcopyrite–bornite–sphalerite, and calcite–galena–sphalerite in the sulfide episode, and chalcedony–limonite in the supergene episode. Re–Os and ⁴⁰Ar–³⁹Ar dating indicates that both the skarn-type and porphyry-type orebodies of the Yinjiagou deposit formed approximately 143 Ma ago during the Early Cretaceous. Four types of fluid inclusions (FIs) have been distinguished in quartz phenocryst, various quartz veins, and calcite vein. Based on petrographic observations and microthermometric criteria the FIs include liquid-rich, gas-rich, H₂O–CO₂, and daughter mineral-bearing inclusions. The homogenization temperature of FIs in quartz phenocrysts of K-feldspar granite porphyry ranges from 341 °C to >550 °C, and the salinity is 0.4–44.0 wt% NaCl eqv. The homogenization temperature of FIs in quartz–molybdenite veins is 382–416 °C, and the salinity is 3.6–40.8 wt% NaCl eqv. The homogenization temperature of FIs in quartz–calcite–pyrite–chalcopyrite–bornite–sphalerite ranges from 318 °C to 436 °C, and the salinity is 5.6–42.4 wt% NaCl eqv. The homogenization temperature of FIs in quartz–molybdenite stockworks is in a range of 321–411 °C, and the salinity is 6.3–16.4 wt% NaCl eqv. The homogenization temperature of FIs in quartz–sericite–pyrite is in a range of 326–419 °C, and the salinity is 4.7–49.4 wt% NaCl eqv. The ore-forming fluids of the Yinjiagou deposit are mainly high-temperature, high-salinity fluids, generally with affinities to an H₂O–NaCl–KCl ± CO₂ system. The δ¹⁸O_H2O values of ore-forming hydrothermal fluids are 4.0–8.6‰, and the δD_V-SMOW values are between −64‰ and −52‰, indicating that the ore-forming fluids were primarily magmatic. The δ³⁴S_V-CDT values of sulfides range between −0.2‰ and 6.3‰ with a mean of 1.6‰, sharing similar features with deeply sourced sulfur, implying that the sulfur mainly came from the lower crust composed of poorly differentiated igneous materials, but part of the heavy sulfur came from the Guandaokou Group dolostone. The ²⁰⁶Pb/²⁰⁴Pb, ²⁰⁷Pb/²⁰⁴Pb, and ²⁰⁸Pb/²⁰⁴Pb values of sulfides are in the range of 17.331–18.043, 15.444–15.575, and 37.783–38.236, respectively, which is generally consistent with the Pb isotopic signature of the Yinjiagou intrusion, suggesting that the Pb chiefly originated from the felsic–intermediate intrusive rocks in the mine area, with a small amount of lead from strata. The Yinjiagou deposit is a porphyry–skarn deposit formed during the Mesozoic transition of a tectonic regime that is EW-trending to NNE-trending, and the multiepisode boiling of ore-forming fluids was the primary mechanism for mineral deposition.  相似文献   

Jump conditions and dynamic surface tension at permeable interfaces such as the inner core boundary     

《Comptes Rendus Geoscience》2014,346(5-6):110-118

We consider a fluid crossing a zone of rapid density change, so thin that it can be considered as a density jump interface. In this case, the normal velocity undergoes a jump. For a Newtonian viscous fluid with low Reynolds number (creeping flow) that keeps its rheological properties within the interface, we show that this implies that the traction cannot be continuous across the density jump because the tangential stress is singular. The appropriate jump conditions are established by using the calculus of distributions, taking into account the curvature of the interface as well as the density and viscosity changes. Independently of any intrinsic surface tension, a dynamic surface tension appears and turns out to be proportional to the mass transfer across the interface and to a coefficient related to the variations of density and viscosity within the interface. Explicit solutions are exhibited to illustrate the importance of these new jump conditions. The example of the Earth's inner core crystallisation is questioned.  相似文献   

http://www.sciencedirect.com/science/article/pii/S1674987114000395     

Alfons van den Kerkhof  Andreas Kronz  Klaus Simon 《地学前缘(英文版)》2014,5(5):683-695

The study of fluid inclusions in high-grade rocks is especially challenging as the host minerals have been normally subjected to deformation, recrystallization and fluid-rock interaction so that primary in- clusions, formed at the peak of metamorphism are rare. The larger part of the fluid inclusions found in metamorphic minerals is typically modified during uplift. These late processes may strongly disguise the characteristics of the ＂original＂ peak metamorphic fluid. A detailed microstructural analysis of the host minerals, notably quartz, is therefore indispensable for a proper interpretation of fluid inclusions. Cathodoluminescence （CL） techniques combined with trace element analysis of quartz （EPMA, LA- [CPMS） have shown to be very helpful in deciphering the rock-fluid evolution. Whereas high-grade metamorphic quartz may have relatively high contents of trace elements like Ti and A1, low- temperature re-equilibrated quartz typically shows reduced trace element concentrations. The result- ing microstructures in CL can be basically distinguished in diffusion patterns （along microfractures and grain boundaries）, and secondary quartz formed by dissolution-reprecipitation. Most of these textures are formed during retrograde fluid-controlled processes between ca. 220 and 500 ℃, i.e. the range of semi-brittle deformation （greenschist-facies） and can be correlated with the fluid inclusions. In this way modified and re-trapped fluids can be identified, even when there are no optical features observed under the microscope.  相似文献   

Complex vein systems as a data source in tectonics: An example from the Ugab Valley,NW Namibia     

《Journal of Structural Geology》2014

Neoproterozoic metaturbidites in the Lower Ugab Domain, Namibia, contain a complex network of four sets of quartz-calcite veins, overprinted by km-scale folds associated with four regional foliations. The veins formed by fluid overpressure predating the main deformation. Deformation structures developed at the junction of two mobile belts during the assembly of Gondwana, the NS Kaoko Belt, and the EW trending Damara Belt. Km-scale NS trending folds were initiated during EW constriction in the Kaoko Belt, while their further development and all subsequent events are related to constriction in the EW-Damara Belt, with coeval sinistral strike slip in the Kaoko Belt. Deformation of the veins, and development of four orthogonal foliations are due to gradual changes in the bulk tectonic framework rather than separate orogenic events. The veins are deformed in a complex manner allowing a full 3D reconstruction of regional sequence of events. The local complex tectonics could be reconstructed because of the perfect local exposure and the multitude of veins: it illustrates the potential complexity of tectonic events and structural evolution in apparently simple slate belts.  相似文献   

Influence of carbonate facies on fault zone architecture     

《Journal of Structural Geology》2014

Normal faults on Malta were studied to analyse fault propagation and evolution in different carbonate facies. Deformation of carbonate facies is controlled by strength, particle size and pore structure. Different deformation styles influence the damage characteristics surrounding faults, and therefore the fault zone architecture. The carbonates were divided into grain- and micrite-dominated carbonate lithofacies. Stronger grain-dominated carbonates show localised deformation, whereas weaker micrite-dominated carbonates show distributed deformation. The weaker micrite-dominated carbonates overlie stronger grain-dominated carbonates, creating a mechanical stratigraphy. A different architecture of damage, the ‘Fracture Splay Zone’ (FSZ), is produced within micrite-dominated carbonates due to this mechanical stratigraphy. Strain accumulates at the point of juxtaposition between the stronger grain-dominated carbonates in the footwall block and the weaker micrite-dominated carbonates in the hanging wall block. New slip surfaces nucleate and grow from these points, developing an asymmetric fault damage zone segment. The development of more slip surfaces within a single fault zone forms a zone of intense deformation, bound between two slip surfaces within the micrite-dominated carbonate lithofacies (i.e., the FSZ). Rather than localisation onto a single slip surface, allowing formation of a continuous fault core, the deformation will be dispersed along several slip surfaces. The dispersed deformation can create a highly permeable zone, rather than a baffle/seal, in the micrite-dominated carbonate lithofacies. The formation of a Fracture Splay Zone will therefore affect the sealing potential of the fault zone. The FSZ, by contrast, is not observed in the majority of the grain-dominated carbonates.  相似文献