湖南香花岭锡多金属矿床同位素地球化学研究

笔者对湖南香花岭锡多金属矿床成矿期不同的矿物组合进行矿物包裹体温度和硫、铅同位素测定,获得了锡石-硫化物阶段平均-温度为350℃,硫化物阶段平均均-温度为250℃.锡石-硫化物中黄铁矿的δ34为-1.O‰～+5.4‰;闪锌矿的δ34S为+0.8‰-+5.8‰;磁黄铁矿的δ34S为+1.5‰～5.2‰;方铅矿的δ34S为-1.0‰+3.6‰,具有变化范围小,组成稳定的特点.方铅矿的206Pb/204Pb值为17.785～19.341,207Pb/204Pb值为15.416～16.452,208Pb/204Pb值为38.357～42.579.硫同位素指示硫来源于岩浆,铅同位素指示是多来源.     

新疆霍什布拉克铅锌矿床硫铅同位素地球化学研究

对新疆霍什布拉克铅锌矿床硫化物硫、铅同位素测定,获得成矿早期黄铁矿的δ34S值为-12.1‰～-8.5‰,闪锌矿的δ34S值为-17.6‰,方铅矿的δ34S值为-18.8‰;晚期黄铁矿的δ34S值为+12.8‰～+22.2‰,闪锌矿的δ34S值为+20.0‰～+24.2‰,方铅矿的δ34S值为+14.4‰+22.2‰.成矿从早到晚,硫同位素由大的负值变化到大的正值,方铅矿的206 Pb/204 Pb比值为17.900-18.086,207Pb/204Pb比值为15.586-15.732,208Pb/204Pb比值为37.997-38.381;黄铁矿的206Pb/204Pb比值为17.950,207 pb/204Pb比值为15.633,208 pb/204 Pb比值为38.144.灰岩的206pb/204 Pb比值为18.156-18.875,207Pb/204Pb比值为15.396-15.855,208Pb/204Pb比值为37.631-38.967.硫同位素指示硫来源于海水硫酸盐还原硫.铅同位素指示至少有两上以上来源.     

广西高龙微细浸染型金矿床同位素地球化学研究

对广西高龙微细浸染型金矿床矿石和脉石矿物进行硫、铅、氢、氧同位素测定,获得沉积岩中黄铁矿的δ34S为-15.3‰～+13.6‰,含矿层中的黄铁矿δ34S值为+0.4‰～+15.6‰,硅质岩中黄铁矿的δ34S为+1.7‰～+9.7‰,硅质岩中辉锑矿的δ34S值为-15.3‰～+0.1‰.从含矿层到硅质岩的黄铁矿,再到硅质岩的辉锑矿,硫同位素组成有降低趋势.黄铁矿的206Pb/204Pb值为8.270～18.470;207Pb/204Pb值为5.620～15.710;208Pb/204Pb值为8.310～38.740.矿床石英的氧同位素为+11.3‰～+23.9‰,水的氧同位素为-4.2‰～+14.4‰,矿物包裹体的氢同位素为-53.4‰～-77.1‰,方解石的氧同位素为+10.5‰～+18.6‰,换算成水中氧同位素为-3.2‰～+10.7‰,氢同位素为-54.5‰～-30.5‰,表明热液可能来源于岩浆热液与大气降水和海水混合.     

新疆可可塔勒铅锌矿床形成硫铅同位素地球化学证据

对新疆可可塔勒铅锌矿床物理化学条件和硫铅同位素研究,获得矿床形成温度为300℃;logfo2为-32.75～-33.91; logf2为-6.75～-10.00;pH值为5.3～7.0.矿石和脉石的206 Pb/204Pb比值为18.001～18.200,207pb/204 Pb比值为15.480～15.705,208Pb/204 Pb比值为37.605～38.861.硫化物的206Pb/204Pb比值为18.001～18.176,207pb/204 Pb比值为15.480～15.634,208Pb/204 Pb比值为37.605～38.027;铁帽的206Pb/204Pb比值为18.017～18.200,207pb/204Pb比值为15.509～15.617,208pb/204 Pb比值为37.833～38.283;重晶石和石英的206 pb/204 Pb比值为18.014～18.027,207pb/204 Pb比值为15.482～15.495,208Pb/204Pb比值为37.632～37.675.硫化物的δ34S值为-15.8‰～+5.1‰,其中黄铁矿的δ34S值为-14.3‰～+5.1‰,方铅矿的δ34S值为-15.8‰～-1.0‰,磁黄铁矿的δ34S值为-14.6‰～-1.4‰,闪锌矿的δ34S值为-14.5‰～-11.3‰.硫同位素指示硫来源于岩浆,铅同位素指示铅是多来源.     

安徽水竹岭铜-铁-金-硫矿床同位素地球化学特征

水竹岭铜-铁-金-硫矿床发育上部层状矿体和下部脉状矿体。上部层状矿石重晶石δ34S值为+19.9‰。上部层状矿石黄铁矿δ34S值为+0.9～+5.8‰,下部脉状矿石黄铁矿δ34S值为+3.2～+6.4‰。下部脉状矿体中方解石的δ18O值为+13.3‰,δ13C值为1.2‰,上部层状矿石白云石的δ18O值为+14.1‰,δ13C值为2.2‰。下部脉状矿石和矿化岩石中黄铁矿的206Pb/204Pb、207Pb/204Pb、208Pb/204Pb平均值分别为18.2241、15.5245和38.2289;上部层状矿石中黄铁矿的206Pb/204Pb、207Pb/204Pb、208Pb/204Pb平均值分别为18.0692、15.5020和38.1232。从下部脉状矿石到上部层状矿石,黄铁矿的δ34S值、206Pb/204Pb、207Pb/204Pb、208Pb/204Pb平均值逐渐降低,δ18O值和δ13C值等逐渐增高。地质和同位素地球化学特征反映水竹岭铜-铁-金-硫矿床为海底热水喷流沉积成因,揭示了块状硫化物矿床的二元结构性。     

内蒙古拜仁达坝及维拉斯托银多金属矿床的硫和铅同位素研究

拜仁达坝和维拉斯托是近年来在内蒙古东部地区发现的2个大型银多金属矿床,文章对其开展了硫和铅同位素研究。结果表明,拜仁达坝矿床矿石中硫化物的δ34S值为-4.0‰～+1.6‰,维拉斯托矿床矿石中硫化物的δ34S值为-0.8‰～+2.0‰,与岩浆热液型矿床的硫同位素值接近,表明这2个矿床中的硫主要来自岩浆。拜仁达坝矿区43件金属硫化物的206Pb/204Pb值为18.333～18.515,207Pb/204Pb值为15.532～15.656,208Pb/204Pb值为38.057～38.610;维拉斯托矿区20件金属硫化物的206Pb/204Pb值为18.304～18.377,207Pb/204Pb值为15.520～15.610,208Pb/204Pb值为38.112～38.435。拜仁达坝东矿区矿石中的铅同位素组成与维拉斯托矿区相似,变化范围小,相对贫放射性铅同位素,并且均为混合铅。矿石中的铅可能来自围岩地层及深源岩浆。     

中条山铜矿床同位素地球化学研究

笔者对中条山绛县群和中条群主要铜矿床进行铅、硫、碳、氢、氧同位素测定，获得：横岭关型矿床的206Pb/204Pb比值为17.746~19.270, 207Pb/204Pb比值为15.500~15.684，208 Pb/204Pb比值为37.236~39.931,硫化物的δ34S值为-8.1‰~+36.9‰, δ18OH2O值为+1.7‰~+5.7‰, δD值为-58. 4‰~-111.3‰；铜矿峪型矿床的206Pb/204Pb比值为18.040~46.243 207Pb/204Pb比值为15.565~18.765,208Pb/204Pb比值为37.682~69.623,硫化物的产δ34S值为-7.2‰～+10.2‰, δ18OH2O为+6.3‰～+10.5‰, δD值为-52.8‰~-123.3‰;落家河型矿床的206Pb/204Pb比值为17.591~19.270, 207Pb/204Pb比值为15.494~15.684,208Pb/204Pb比值为37.263~39.931,硫化物的δ34S值为-1‰~-21.9‰, δ18OH2O值为+3.6‰~+6.4‰, δD值为-35.8‰~-70‰;胡-蓖型矿床206 Pb/204 Pb比值为18.097~249.50, 207Pb/204Pb比值为15.578~44.230,208Pb/204Pb比值为35.379~51.480,硫化物的δ34S值为3.4‰~23.2‰, δ18OH2O值为+7.5‰~+12.5‰, δD值为-36.3‰~-72.2‰。     

凡口铅锌矿床同位素地球化学证据

对凡口铅锌矿床不同成矿阶段进行矿物包裹体温度、硫和铅同位素测定，获得成矿第Ⅰ阶段温度为300±50℃，第Ⅱ、Ⅲ阶段温度为250±50℃；并获得矿床硫化物的S同位素组成为2.1‰～26.5‰，具有δ34SPy＞δ34SSp＞δ34SGn；第Ⅰ阶段硫化物的硫同位素组成随赋存层位由老到新硫同位素有逐渐减小趋势；第Ⅱ阶段硫化物的δ34S为14.3‰～23.8‰；第Ⅲ阶段硫化物的δ34S为5.7％~15.7‰，具有从早阶段至晚阶段硫同位素组成变化范围从大至小的减小趋势。分析获得68件铅同位素数据，其中硫化物的206Pb/204Pb比值为18.023～18.847；207Pb/204Pb比值为15.700～15.820；208Pb/204Pb比值为38.056～39.796。灰岩全岩的206Pb/204Pb比值为18.230～18.860；207Pb/204Pb比值为15.640～16.000；208Pb/204Pb比值为38.714～39.960。辉绿岩的206Pb/204Pb比值为18.570～18.650；207Pb/204Pb比值为15.260～15.620；208Pb/204Pb比值为38.650～38.960。第Ⅰ阶段δ34OH2O为13.3‰~13.1‰，δD为－50.2‰～－61.5‰；第Ⅱ阶段δ18OH2O为－2.4‰～＋10.8‰，δD为－50.2‰～－63.2‰；第Ⅲ阶段δ18OH2O为－4.9‰～－14.3‰，δD为－59.0‰～－61.0‰。     

滇西北雪鸡坪斑岩铜矿S,Pb同位素组成及对成矿物质来源的示踪

雪鸡坪斑岩铜矿位于西南三江构造火成岩带义敦岛弧带,其成矿斑岩为印支期石英闪长玢岩和石英二长斑岩。研究对该矿区安山岩、矿化斑岩和矿石矿物系统进行S,Pb同位素分析结果表明:金属硫化物的δ34S值为-3.1‰～ 0.7‰,平均值为-1.1‰,与矿化斑岩的硫同位素组成(-1.4‰和-1.5‰)一致,均落入幔源硫范围,表明硫主要来自岩浆;δ34S黄铁矿(-1.8‰～ 0.7‰,平均-0.5‰)>δ34S黄铜矿(-2.2‰～0.0‰,平均-1.2‰)>δ34S方铅矿(-3.1‰～-1.3‰,平均-2.4‰),硫同位素分馏基本达到平衡。矿石矿物(208Pb/204Pb=37.917～38.230,平均值38.075;207Pb/204Pb=15.528～15.614,平均值15.571;206Pb/204Pb=17.929～18.082,平均值17.981)与矿化斑岩(208Pb/204Pb=37.832、37.883,207Pb/204Pb=15.529、15.538,206Pb/204Pb=17.906、17.910)以及安山岩(208Pb/204Pb=37.816～37.884,207Pb/204Pb=15.549～15.562,206Pb/204Pb=17.845～17.919)的初始铅组成基本一致,变化范围较小,表明三者具有相同的来源;在铅构造模式图上,所有样品铅同位素均位于造山带演化线上或附近,在铅同位素源区判别图中,均落入造山带和下地壳区域,这表明Pb主要来源于壳幔混合。雪鸡坪铜矿S,Pb同位素组成共同指示成矿物质主要来自于深部岩浆,这种岩浆可能主要起源于俯冲洋壳板片的部分熔融并受到少量地壳物质的混染。     

湘南宝山铅锌矿床硫、铅、碳、氧同位素特征及成矿物质来源

宝山铅锌矿床是湘南地区代表性矿床之一。宝山铅锌矿床的成矿作用与156~158 Ma的宝山花岗闪长斑岩密切相关。花岗闪长斑岩主要由古老地壳部分熔融而成。为确定成矿物质来源,文章系统研究了宝山铅锌矿床的硫、铅、碳、氧同位素组成特征。矿床中硫化物黄铁矿、闪锌矿、方铅矿的δ34S值呈狭窄的塔式分布,变化在-2.17‰~6.46‰之间,平均值为3.13‰。δ34S值总体表现为δ34S黄铁矿δ34S闪锌矿δ34S方铅矿,表明硫同位素分馏基本达到了平衡。矿石、花岗闪长斑岩和赋矿地层硫同位素对比研究表明,矿石中的硫主要由岩浆分异演化而来,岩浆中的硫主要来自古老地壳。矿石206Pb/204Pb、207Pb/204Pb和208Pb/204Pb比值分别为18.188~18.844、15.661~15.843和38.562~39.912,赋矿地层206Pb/204Pb、207Pb/204Pb和208Pb/204Pb比值分别为18.268~19.166、15.620~5.721和38.364~39.952。矿石铅同位素组成比地层中的更富放射性成因铅,矿石中部分铅来自宝山花岗闪长质岩浆,在成矿流体运移过程中有部分地层铅参与了成矿,岩浆中的铅主要来自古老地壳。热液方解石的碳、氧同位素组成介于岩浆和赋矿碳酸盐岩的碳、氧同位素之间,主要是由于岩浆流体和碳酸盐岩不同比例的水岩反应所致,测水组有机碳的加入造成了部分热液方解石δ13CPDB值偏低。     

岩石坚硬程度对核电厂地基-基础地震响应特征的影响分析

考虑核电厂地基-基础的动力相互作用,应用显式动力有限差分法分析了地震作用下极软岩、较软岩、坚硬岩上核电厂建筑结构基础的地震响应特征,比较了岩石坚硬程度对基础加速度反应谱的影响。研究表明：随着岩石坚硬程度的提高,核电厂建筑物结构基础的地震响应有增加的趋势;在周期轴上,基础处的加速度反应谱曲线会随着岩石坚硬程度的提高逐渐向短周期（高频段）方向移动。在高频段,建造于较坚硬岩石上基础结构的加速度反应谱值偏大;在中等频段,建造于较软岩石上基础结构的加速度反应谱值偏大;在低频段,岩石坚硬程度对加速度反应谱的影响不显著。     

Geochemistry of Thermal Waters of Continental Margin of Far East of Russia

Studied waters belong to warm(T=30-50℃),alkaline(pH=8.9-9.3),low mineralized(TDS235 mg/1)Na-HCO_3 or Na-SO_4-HCO_3 thermal waters with high content of SiO_2(up to 81 mg/l)and F(up to 3.9 mg/1),occur on modern volcano-tectonic rejuvenated areas of Eastern Sikhote-Alin orogenic belt.Low~3He concentration as well as N_2/O_2 and N_2/Ar ratios exclude influence of deep mantle fluid.New rare earth element data constrain our understandmg of water-rock interaction occurring in the water source region.Meteoric origin of waters is proved by stable isotope values varying from-71‰to-136.1‰and from-10.8‰to-18.8‰forδ~2U andδ~(18)O respectively.REE patterns reflect high pH,resultfing from water-rock interaction and oxidative conditions.Calculations of deep aquifer temperature using Na-K and quartz geothermometers show 116.8-131.1°C and 82.2-125.8℃respectively.Presence of deep faults both with abnormal thermal gradient(~45-50 K/km)define unique geochemical shape of thermal waters of Sikhote-Alin,area,where no present volcanic activity is registered.     

Strains of scattering of near-field of a point source

Three dimensional scattering of near-field is studied for dilatation and rotation in the time domain. The perturbation method is applied to solve the equation of motion for the first order scattering from a weak inhomogeneity in an otherwise homogeneous medium. The inhomogeneity is assumed close enough to the point source so that the near-field intermediate wave is dominating over the far-field sphericalP andS pulses. The integral expressions are derived to relate dilatation and rotation of scattering to the radial fluctuations of velocities and density in the inhomogeneity. These integrals are solved to calculate the strains of scattering from (a part of) an inhomogeneous spherical shell of arbitrary curvature. Variable curvature may allow the shape of inhomogeneity volume element to change uniformly from spherical to rectangular. Rotation of scattering from a spherical shell is independent ofP wave velocity inhomogeneity. Dilatation of scattering does not involveS wave velocity inhomogeneity but its gradient. The back scattering results are obtained as a special case. Strains are computed numerically, for hypothetical models to study the effects of various parameters viz., velocity inhomogeneity, distance of source from inhomogeneity and from receiver, and thickness of inhomogeneity. The curvature of the spherical shell is varied to study the effects of the shape of inhomogeneous volume element on scattering.     

土石坝心墙水力劈裂分析

简要分析了水力劈裂的发生条件、力学机理。基于水压楔劈机理,利用有限元方法建立了一种水力劈裂的发生判定方法。该方法假定心墙预先存在局部渗透弱面（裂缝）,通过将裂缝位置的单元材料改为裂缝软材料,考虑库水进入裂缝后对裂缝周围土体的作用,建立水力劈裂分析的平面有限元模型,确定裂缝端部垂直于裂缝面的正应力,进而依据该正应力判断水力劈裂发生的可能性,该方法同时可模拟水力劈裂的发展过程。     

土钉支护失稳分析

某基坑采用复合土钉墙支护,开挖至坑底后,基坑北侧发生失稳事故。本文就其事故发生原因作一探讨。     

地震次生地质灾害风险评估集对态势分析

5．12四川汶川8级强震引发了大量次生地质灾害,加剧了灾情并严重影响抗震救灾。地震次生地质灾害受多重因素制约,其孕育与致灾过程具有不确定性。利用集对分析原理与方法,对地震次生地质灾害进行同异反态势分析,拟定了风险评估的集对分析同一度、差异度、对立度等指标体系的构建原则与赋值标准,对承灾体系统的不确定性及其作用作了刻画与分析,建立了不同风险分区代表性的集对分析联系度表达式,为地震灾害研究提供了可资借鉴的新思路和技术方法。     

下扬子区三叠纪古地理演化

下扬子区在三叠纪期间接受了早-中三叠世海相碳酸盐沉积、中-晚三叠世海陆交互相和陆相湖沼沉积.沉积相带的空间分布和古地理格局的变迁明显地受到区域构造的控制.区内盆地发育与演化是在华南板块与扬子板块、扬子板块与华北板块相互作用的背景下进行的.早-中三叠世末期的印支运动是下扬子区构造-古地理格局改变的决定性因素,使下扬子海盆闭合,沉积类型由海相沉积变为陆相沉积.下扬子区三叠纪古地理的演化特征也为板块碰撞提供了沉积证据.     

多年冻土融沉性分类研究

在冻土工程中,冻土的融沉性评价是工程地质勘察的主要内容之一,融沉性分类是冻土地基基础设计施工的重要依据．根据345个冻土原状样品融沉压缩试验数据,提出了细砾、砂土、粉土、黏性土、泥炭化黏性土和泥炭质土等6类土的融沉系数一含水量或融沉系数一超塑含水量线性回归方程式,得到与各融沉性分级相应的界限含水量或界限超塑含水量．最后...     

Kinetics of dehydration of Ca-montmorillonite

Isothermal thermogravimetric experiments have been carried out to determine the reaction kinetics of the dehydration processes in fuller's earth, a natural Ca-montmorillonite. Dehydration in swelling clays is a complex reaction, and analysis of the thermogravimetric data using empirical rate equations and time-transformation analysis reveals that the nature of the rate controlling mechanism is dependent upon both the temperature regime of the sample as well as the extent of reaction. For fuller's earth, we find that the dehydration kinetics are dominated by a nucleation and growth mechanism at low temperatures and fractions transformed (stage I), but above 90 °C the last stages of the reaction are diffusion controlled (stage II). The activation energy for dehydration during stage I is around 35 kJ · mol⁻¹, whereas the removal of water during stage II requires an activation energy of around 50 kJ · mol⁻¹. These two stages of dehydration are associated with primary collapse of the interlayer (stage I) and movement of water that is hydrated to cations within the interlayer (stage II). Received: 28 August 1998 / Revised, accepted: 27 January 1999