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121.
福建省水系沉积物微量元素含量特征及成矿远景预测   总被引:6,自引:0,他引:6  
林才浩  尤爱珍 《地质与勘探》1996,32(5):33-36,41
根据区域化探水系沉积物测量分析3万余件样品中40种元素含量,统计了32种微量元素的背景平均值,浓度克拉克值,总体变化系数等参数。在利用水系沉积物富集系数估计值对浓度克拉克值进行校正后,使用顺序号累加法对福建省32种元素内生成矿作用的规模进行预测排序,并分析了银,硼的资源潜力。  相似文献   
122.
刘纲 《黄金地质》1996,2(4):43-49
系统论述了区内各大类金矿的成矿温度,成矿压力,各种气体的逸度、pH值,金离子及其配合物的活度,讨论了金的迁移形式,推测了区内各类矿液中金的沉淀机制。  相似文献   
123.
A new method for solving the transport equation based on the management of a large numbe of particles in a discretized 2-D domain is presented. The method uses numerical variables to represent the number of particles in a given mesh and is more complex than the 1-D problem. The first part of the paper focuses on the specific management of particles in a 2-D problem. The method also would be valid for three dimensions as long as the medium can be modeled similar to a layered system. As the particles are no longer tracked individually, the algorithm is fast and does not depend on the number of particles present. The numerical tests show that the method is nearly numerical dispersion free and permits accurate calculations even for simulations of low-concentration transport. Because each mesh is considered as a closed system between two successive time steps, it is easy to add adsorption phenomenon without any problem of numerical stability. The model is tested under conditions that are extremely demanding for its operating mode and gives a good fit to analytical solutions. The conditions in which it can be used to best advantage are discussed.  相似文献   
124.
流体地质作用的构造效应   总被引:2,自引:1,他引:2  
许多事实证明,在地壳及地球深部存在着大量的流体,它们以气体、液体、熔融体等形式存在于地球内部不同深度处。这些流体的活动在地壳及岩石圈运动演化过程中扮演着十分重要的角色,其作用贯穿于地壳与岩石圈运动演化的全过程,地球表面形成的各种构造与流体作用的参与有着密切的联系。  相似文献   
125.
着重总结了我国古大陆及其边缘早古生代大层序(megasequence,一级层序)和中层序(mesosequence,二级层序),以及一级、二级海平面变化的基本特征,并与国外早古生代海平面变化进行对比.我国3大古陆(华北陆块、扬子陆块、塔里木陆块)及其边缘早古生代大层序可划分为两个(MG-1,MG-2).中层序划分为5个(MS-1,MS-2,MS-3,MS-4,MS-5).MG-1包括MS-1,MS-2和MS-3,时限为94~112Ma(寒武纪和早奥陶世),底以巨大不整合为界,顶以著名巨大沉没不整合为限,沉积了我国显生宙大部分的碳酸盐岩,赋存着丰富的油气和各种金属及非金属矿产.MG-2包括MS-4和MS-5,时限为58~68Ma(中、晚奥陶世和志留纪),底界以巨大沉没不整合为界,为硅质碎屑-碳酸盐岩组合.海平面变化的级别划分对应于层序.中国3大古陆及其边缘早古生代海平面变化的总貌:MGSC-1初期普遍发生快速海进,海平面升高,尔后海平面下降,其间有多期次的小幅度海进和海退变化.MGSC-2则普遍海平面升高,上升幅度大于MGSC-1,尔后逐渐下降.  相似文献   
126.
对对流占优的三维溶质运移问题提出了分步广义迎风解法,首先利用N.N.Ya-nenko对水动力弥散方程分步求解的思想,将原来的一个定解问题分解为两个定解问题即对流定解问题和扩散定解问题,对对流定解问题采用广义迎风对偶单元均衡法求解,对扩散定解问题采用一般的Galerkin有限元法求解,不仅避免了用一般有限元法和有限差分法求解对流占优的地下水水质数学模型时常出现数值弥散和过量问题,而且避免了求节点速度这一步,节省运算步骤,对井点的浓度变化给出了更合适的求解方法。  相似文献   
127.
The Changkeng gold-silver deposits consist of a sediment-hosted, disseminated gold deposit and a replacement-type silver deposit. The mineralizations of gold and silver are zoned and closely related to the silicification of carbonate and clastic rocks, so that siliceous ores dominate in the deposit. The mineralizing temperature ranges mainly from 300 to 170℃, and K+, Na+, Ca2+, Mg2+, and Cl- are the major ions in the ore-forming fluid. Calculations of distribution of metal complexes show that gold is mainly transported by hydrosulphide complexes, but chloride complexes of silver, iron, lead, and zinc, which are transformed into hydroxyl and hydrosulphide complexes under neutral to weak-alkaline circumstances in the late stage, predominate in the ore-forming solutions. Water-rock interaction is confirmed to be the effective mechanism for the formation of silver ores by computer modelling of reaction of hydrothermal solution with carbonate rocks. The solubility analyses demonstrate that the precipitation  相似文献   
128.
Large-eddy simulations of a clear convective boundary layer (CBL)and a stratocumulus-topped boundary layer are studied. Bottom-upand a top-down scalars were included in the simulations, and theprinciple of linear superposition of variables was applied toreconstruct the fields of any arbitrary conserved variable.This approach allows a systematic analysis of countergradient fluxesas a function of the flux ratio, which is defined as the ratio betweenthe entrainment flux and the surface flux of the conserved quantity.In general, the turbulent flux of an arbitrary conserved quantityis counter to the mean vertical gradient if the heights where thevertical flux and the mean vertical gradient change sign do notcoincide. The regime where the flux is countergradient is thereforebounded by the so-called zero-flux and zero-gradient heights. Becausethe vertical flux changes sign only if the entrainment flux has anopposite sign to the surface flux, countergradient fluxes arepredominantly found for negative flux ratios. In the CBL the fluxratio for the virtual potential temperature is, to a good approximation,constant, and equal to -0.2. Only if the moisture contribution to thevirtual potential temperature is negligibly small will the flux ratio forthe potential temperature be equal to this value. Otherwise, theflux ratio for the potential temperature can have any arbitrary(negative) value, and, as a consequence, the fluxes for thepotential temperature and the virtual potential temperature willbe countergradient at different heights. As a practical application ofthe results, vertical profiles of the countergradient correction termfor different entrainment-to-surface-flux ratios are discussed.  相似文献   
129.
130.
During bedload movement by saltation, streamwise momentum is transferred from the ?ow to the saltating grains. When the grains collide with other grains on the bed or in the ?ow, streamwise momentum is reduced, and there is a decrease in streamwise ?ow velocity and an increase in ?ow resistance, herein termed bedload transport resistance fbt. Based on experiments in two ?umes with ?xed and mobile plane beds and previously published data, an equation is developed that may be used to predict fbt for both capacity and non‐capacity ?ows. The variables in this equation are identi?ed by dimensional analysis and the coef?cients are determined by non‐linear regression. This equation applies to rough turbulent open‐channel ?ows, where the relative submergence is between 1 and 20 and the entire sediment load moves by saltation. An investigation of the relative magnitudes of fbt and grain resistance fc suggests that where dimensionless shear stress θ is less than 1 and saltation is the dominant mode of bedload transport, fbt/fc increases with θ but never exceeds 1. Copyright © 2004 John Wiley & Sons, Ltd.  相似文献   
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