青海索拉沟银多金属矿床成矿特征及成因探讨

索拉沟地区位于青海省东昆仑东部与西秦岭造山带的接合部位,地质构造复杂,岩浆活动较强烈,成矿背景条件良好,是青海省贵金属、铜多金属重要的成矿带之一。根据矿床产出的地质构造环境、成矿特征、矿物组成、电子探针、流体包裹体温压测试及元素组合等特点分析,推测矿床的形成经历了热水沉积成矿和热液叠加改造成矿,索拉沟银多金属矿为热水沉积-热液叠加改造型。     

胶东地区与金矿成矿有关的花岗岩体中的流体包裹体研究

与胶东金矿有密切关系的玲珑片麻状花岗岩、栾家河二长花岗岩、郭家岭花岗闪长岩、上庄二长花岗岩4种类型花岗岩中矿物包裹体的发育程度、类型、大小及其特点, 以及包裹体的显微测温结果, 反映出玲珑岩体是经历了高级区域变质作用形成的重熔型花岗岩, 郭家岭岩体是由高温、高粘度岩浆结晶成岩的。栾家河岩体是由一种富CO₂的高温、高粘度的岩浆中结晶演化而来, 岩体的侵入深度也较浅。上庄岩体形成温度压力较低。      

豫西银家沟硫铁多金属矿床流体包裹体和同位素特征

河南省银家沟硫铁多金属矿床位于华北克拉通南缘华熊地块内,是东秦岭地区最大的硫铁多金属矿床,以其硫铁储量大及共、伴生元素复杂区别于东秦岭其他以钼为主的矿床.成矿的全过程可以划分为矽卡岩期、硫化物期和表生期,包括磁铁矿阶段、脉状石英-辉钼矿阶段、石英-黄铁矿-黄铜矿-斑铜矿-闪锌矿阶段、网脉状石英辉钼矿阶段、石英绢云母-黄铁矿阶段、方解石-方铅矿闪锌矿阶段和玉髓褐铁矿阶段.流体包裹体研究表明,银家沟矿床主要发育气液两相水溶液包裹体(W型)、含CO2三相包裹体(C型)和含子矿物多相包裹体(S型).钾长花岗斑岩的石英斑晶中流体包裹体均一温度介于341～＞550℃之间,盐度介于0.4％～44.0％ NaCl eqv之间,属H2O-NaCl-CO2体系;脉状石英-辉钼矿阶段流体包裹体均一温度介于382～416℃之间,盐度介于3.6％～40.8％ NaCl eqv之间,属H2O-NaCl体系;石英-方解石-黄铁矿黄铜矿-斑铜矿-闪锌矿阶段流体包裹体均一温度介于318～436℃之间,盐度介于5.6％～42.4％ NaCl eqv之间,属H2O-NaCl体系;网脉状石英-辉钼矿阶段流体包裹体均一温度介于321～411℃之间,盐度介于6.3％～16.4％ NaCl eqv之间,属H2 O-NaCl体系;石英-绢云母黄铁矿阶段流体包裹体均一温度介于326～419℃之间,盐度介于4.7％～49.4％ NaCl eqv之间,属H2O-NaCl体系.银家沟矿床成矿流体主要为高温、高盐度流体,总体上属于H2O-NaCl±CO2体系.成矿热液的δ18 OH2O值为4.0‰～8.6‰,δ18 Dv-SMOW值为-64‰～-52‰,表明成矿流体来自岩浆水.矿石金属硫化物的δ18 SV-CDT值介于-0.2‰～6.3‰之间,平均为1.6‰,具深源硫特征,硫主要来自分异很差的由火成物质组成的下地壳,官道口群白云岩亦提供了部分重硫.矿床金属硫化物的206 Pb/204 Pb值介于17.331～18.043之间,207 Pb/204 Pb值变化于15.444～15.575之间,208 Pb/204 Pb值变化于37.783～38.236之间,总体上与银家沟岩体的铅同位素范围一致,暗示铅主要来自矿区内的燕山期中酸性岩体,地层在成矿过程中亦提供了少量物质.银家沟矿床属斑岩-矽卡岩型,形成于中生代EW向构造体制向NNE向构造体制转变阶段,成矿流体多期次的沸腾作用是矿质沉淀的主要机制.     

福建省地下流体观测干扰因素综合查询系统的设计与实现

将福建省地下流体观测网内观测井各测项在观测期间内出现的干扰事件进行汇总,并进行分类入库保存,实现地下流体干扰因素的录入、查询、检查、修改、计算。编制一个操作界面友好、功能全面的观测井各测项的正常动态与干扰因素综合查询系统,更好地发挥观测数据共享的作用,为分析预报人员查找干扰资料提供方便,同时为福建省地震地下流体观测井的效能评价提供指导作用。     

辽宁省大民屯凹陷流体化学场特征及油气成藏意义

从地层水化学场、油气组成的非均质性两方面对辽宁省大民屯凹陷前第三系古潜山和下第三系沙河街组的流体化学场特征进行了分析.结果表明,该区地层水运动规律与油气运移模式吻合较好,即流体以"垂向流动"为主,受断裂和沉积砂体的控制,由沉积中心的中、深部沿断裂垂向运移,而后在各断块内侧向运移至各断块的高部位,横向运移效应只在局部小范围内规律显著,构成了典型的离心状渗流体系.在地层水水头压力、浮力动力场控制下该区形成了自生自储、下生上储、新生古储型油藏.     

Late Paleozoic Fluid Systems and Their Ore-forming Effects in the Yuebei Basin, Northern Guangdong, China

Based on detailed and systematic researches of the geology of ore deposits, fluid inclusions and isotope geochemistry etc., and regarding the Late Paleozoic fluid system of the Yuebei Basin as an integrated object in this paper, we have revealed the temporo-spatial evolution law of the basin＇s fluid system and discussed its ore-forming effects by simulating and analyzing the distribution of ore-forming elements, the fluid thermodynamics and dynamics of evolution processes of this basin. The results show that Late Paleozoic ore-forming fluid systems of the Yuebei Basin include four basic types as follows. （1） The sea floor volcanic-exhalation system developed during the rapid basin slip-extension stage in the Mid-Late Devonian, which affected the Dabaoshan region. It thus formed the Dabaoshan-type Cu-Pb-Zn-Fe sea floor volcanic-exhalation sedimentary deposits. （2） The compaction fluid system developed during the stable spreading and thermal subsidence-compression stage of the basin in the Mid-Late Devonian. The range of its effects extended all over the whole basin. It resulted in filling-metasomatic deposits, such as the Hongyan-type pyrite deposits and pyrite sheet within the Fankou-type Cu-Pb-Zn-S deposits. （3） The hot water circulation system of sea floor developed during the stage of basin uplifting and micro-aulacogen from the late Late Carboniferous to Middle Carboniferous. The range of its effects covered the Fankou region. It thus formed MVT deposits, such as the main orebody of the Fankou-type Pb-Zn-S deposits. （4） The gravity fluid system developed during the stage of fold uplifting and the basin closed from Middle Triassic to Jurassic, forming groundwater hydrothermal deposits, e.g. the veinlet Pb-Zn-calcite orebodies of the Fankou-type Pb-Zn- S deposits. Migration and concentration of the ore-forming fluids were constrained by the state of temporo-spatial distribution of its fluid potential. Growth faults not only converged the fluids and drove them to move upwards, but also the fluids often crossed the faults to the edges of the basin at the bottom of these faults and the lithologic interfaces, and even migrated to the basin＇s edges from top to bottom along the faults, which may be one of the basic reasons for the stratabound deposits to cluster mainly along the contemporaneous faults on the inner border of the basin. The superposed mineralization resulting from the multi-stage activity of contemporaneous faults and ore-forming fluid systems in the basin may be one of the key factors for forming superlarge ore deposits.     

云南会泽超大型铅锌矿床成因研究中的几个问题

位于川-滇-黔铅锌多金属成矿域中南部云南会泽超大型铅锌矿床可能是一种新的铅锌矿床类型，该类铅锌矿床明显特征是规模大、品位富、伴生有用元素多，暗示其成矿环境较为特殊。从成矿时代、成矿物质来源、成矿流体来源与演化，以及峨眉山玄武岩与成矿的关系等方面分析了会泽超大型铅锌矿床的研究进展及国内外研究现状，认为矿床成矿时代与西南大面积峨眉山玄武岩成矿时代相近，成矿物质和成矿流体具有“多源性”，成矿流体存在均一化过程，区域大规模流体运移在该区铅锌成矿过程中具有重要意义，峨眉山玄武岩岩浆活动与铅锌成矿具有密切的成因联系，矿床可能为“均一化成矿流体贯入成矿”的产物。     

琼东南盆地超压系统泄压带: 可能的天然气聚集场所

泄压带是超压系统内部流体向外运移的通道和有利的油气聚集场所, 对水溶相天然气析离成藏更有着重要意义.本文综合应用速度谱、测井、钻井和地层测试等资料预测了琼东南盆地超压系统的分布, 将其划分为3种结构类型; 结合粘土分析等资料识别出了4种类型的泄压带, 并讨论了泄压带的分布与可能的天然气聚集区带.琼东南盆地中央坳陷带整体发育一个超压系统, 其分布格局主要受陆坡带的形成和莺歌海盆地超压传递的影响, 陆坡区的超压明显强于非陆坡区, 西部的超压整体强于东部并在浅部呈现自西向东传递的趋势.泄压带内的天然气成藏主要取决于压力、温度和溶解气量, 需满足溶解气量足够多和溶解度变化量足够大, 相对而言, Ⅱ型泄压带成藏条件最优, 既有断裂沟通深部水溶气和浅部储层, 又有温压条件的显著变化, 因而流体运移最活跃.Ⅲ型泄压带次之, 但分布最广, 该类型最有利部位分布在陵水低凸起和宝岛凹陷北坡.      

海拉尔盆地乌尔逊凹陷古流体动力场数值模拟

首先对地下水动力场进行数学描述,以水动力为主线,建立适合该地区的数学模型,选择正确的地质模型参数,主要采用数值计算和模拟等手段,在恢复出乌尔逊凹陷主要目的层在不同地质历史时期古水动力的基础上又恢复出古流体势的演化历史。整体上,在乌尔逊凹陷,各主要地质时期的油势演化特征为西部地区大于东部地区,乌南大于乌北,且低势区的发育有较好的继承性。最后,依据油气聚集理论,进行油气运移聚集系统的划分、油气运移方向的分析,从而得出有关研究区油气运移聚集条件的认识,主要从流体动力的角度考虑,指出有利聚集区,认为在乌尔逊凹陷苏4～苏18井区、苏132～苏17～铜2井区及巴1～巴2～巴4井区为有利油气运移聚集区。     

Investigation of a longfin inshore squid's swimming characteristics and an underwater locomotion during acceleration

In the present study, locomotion of a real longfin inshore squid (Doryteuthis pealeii) was numerically investigated. Geometry of a real squid was obtained using computed tomography (CT) images. In addition to a two-dimensional axisymmetric squid model, a modified squid model with no cavities around her head and an ellipse shaped model were generated with a fineness ratio (the ratio of body length to maximum body diameter) of 7.56. These numerical models were exposed to an acceleration with two different velocity programs. Added mass and basset forces on bodies were calculated during acceleration of the squid models starting from rest. Pressure and viscous drag forces were also calculated due to pressure variation along the squid models and friction on the surface of the models. The effect of a nozzle diameter on jet velocities and propulsive efficiency at all bodies were evaluated when time dependent velocity profiles (from 0 to 10 m/s in 0.5 and 1 s time durations) were set for the inlet of computational domain. The modified squid model required least thrust force during acceleration phase of time dependent velocity profile compared to the other models while the 0.02 m nozzle diameter provided largest propulsive efficiency for all models.