A bed‐load transport model for rough turbulent open‐channel flows on plane beds

Data from flume studies are used to develop a model for predicting bed‐load transport rates in rough turbulent two‐dimensional open‐channel flows moving well sorted non‐cohesive sediments over plane mobile beds. The object is not to predict transport rates in natural channel flows but rather to provide a standard against which measured bed‐load transport rates influenced by factors such as bed forms, bed armouring, or limited sediment availability may be compared in order to assess the impact of these factors on bed‐load transport rates. The model is based on a revised version of Bagnold's basic energy equation i_bs_b = e_bω, where i_b is the immersed bed‐load transport rate, ω is flow power per unit area, e_b is the efficiency coefficient, and s_b is the stress coefficient defined as the ratio of the tangential bed shear stress caused by grain collisions and fluid drag to the immersed weight of the bed load. Expressions are developed for s_b and e_b in terms of G, a normalized measure of sediment transport stage, and these expressions are substituted into the revised energy equation to obtain the bed‐load transport equation i_b = ω G ^3·4. This equation applies regardless of the mode of bed‐load transport (i.e. saltation or sheet flow) and reduces to i_b = ω where G approaches 1 in the sheet‐flow regime. That i_b = ω does not mean that all the available power is dissipated in transporting the bed load. Rather, it reflects the fact that i_b is a transport rate that must be multiplied by s_b to become a work rate before it can be compared with ω. It follows that the proportion of ω that is dissipated in the transport of bed load is i_bs_b/ω, which is approximately 0·6 when i_b = ω. It is suggested that this remarkably high transport efficiency is achieved in sheet flow (1) because the ratio of grain‐to‐grain to grain‐to‐bed collisions increases with bed shear stress, and (2) because on average much more momentum is lost in a grain‐to‐bed collision than in a grain‐to‐grain one. Copyright © 2006 John Wiley & Sons, Ltd.     

A Statistical Investigation of the Earthquake Predictions Using LURR

In terms of the spatial scanning of LURR (Load-Unload Response Ratio), we have been predicting the seismic tendency within the next year for the mainland of China from 1995 to 2003. In order to make the quantitative retrospective assessment of LURR method, we compare the results with Poisson null hypothesis. The results show that the prediction by LURR method is much better than Poisson hypothesis.     

西藏普兰石炭纪地层的厘定及其地质意义

通过区域地质调查,利用确定上覆、下伏地层时代与区域地层对比方法,结合邻区古生物年代特征,对西藏普兰北喜马拉雅分区下石炭统进行了厘定。普兰地区早石炭世受沉积环境与物质供应量等因素影响,岩性、岩石组合特征与邻区略有差异,其下部以变质粉晶灰岩为主夹变质泥质粉砂岩,厘定为亚里组;上部以变质细粒砂岩为主夹变质粉晶灰岩,厘定为纳兴组。     

伊犁盆地侏罗系水西沟群层序地层学研究

伊犁盆地侏罗系水西沟群是一套在基本一致的构造应力和沉积环境下形成的含煤碎屑岩建造,但在这套地层的中部(三工河组)出现了岩性、颜色的突变,并且对应的测井曲线也出现明显的突坎现象。笔者运用层序地层学的观点,从年代地层、岩性、体系域、沉积韵律以及测井曲线解释等5方面对这一现象进行了分析,认为该群中部存在一不整合面(或层序界面),并尝试对水西沟群层序地层进行重新划分。     

江西相山邹家山-石洞断裂带及其控矿作用

邹家山石洞断裂构造带(又称邹石构造带)由几组大致平行的断裂组成,总体走向为30°~40°,倾向NW或SE,倾角65°~85°,深切基底达10 km,属区域性NE向走滑断层。根据断裂构造的发育程度、构造联合控矿作用等特点,自北向南将邹石构造带分为石马山段、邹家山段、书塘段和石洞段。研究构造带的铀矿化蚀变特征及构造控矿规律发现,邹石构造带在不同地段控矿形式不同,按容矿位置可分为两类,即主断裂容矿和旁侧次级断裂容矿。邹石构造带的铀矿化作用明显分为两期,邹石构造带附近的铀矿床均存在铀赤铁矿型矿化蚀变,表明邹石构造带对成矿的重要作用。相山矿田各矿床内矿带的展布表明,主要矿带走向的法线方向总是指向相山盆地的特定区域。在总结已知矿床规律的基础上,笔者认为邹石构造带仍然是相山盆地最具找矿潜力的地区之一,书塘地区是邹石构造带的首选找矿靶区。     

潞西盆地浅层地下水脆弱性预测分析

运用DRASTIC方法，评价潞西盆地浅层地下水脆弱性，结合区内人类工程活动因子。对潞西盆地远期地下水脆弱性进行预测分析，成果可为区内土地规划、备用水源地的选择、垃圾填埋场的选址及实现水资源可持续利用提供合理依据。     

内蒙古沙麦岩体：正εNd（t）值的过铝质花岗岩

内蒙古沙麦岩体位于大兴安岭中段西坡,是二连浩特-东乌珠穆沁旗花岗岩带的重要组成部分。岩体中脉岩和围岩捕虏体较为发育,岩性组合主要为中细粒黑云母花岗岩和细粒似斑状花岗岩。在化学成分上,沙麦岩体以铝弱过饱和,富硅,全碱含量中等和低磷为特点,标准矿物中刚玉分子大于1%,可归为过铝质 S 型花岗岩。在稀土元素和微量元素组成上,岩体富 Rb、Th、U、Ta,贫 Ba、Sr、P、Ti,Rb/Sr 比值高,K/Rb 比值低,Eu 负异常明显。在 Nd 同位素组成上,岩体 Nd 同位素组成变化较大,除一件样品ε_(Nd)(t)值为负值以外,普遍以具正ε_(Nd)(t)值为特点,T_(2DM)值介于275.79～1048.41Ma 之间。研究结果表明,沙麦岩体形成于晚中生代后造山的岩石圈伸展环境中,是幔源基性岩浆底侵及其诱发的壳-幔混合岩浆,同化中上地壳泥质围岩并经高程度分离结晶的产物。     

白河黄石板铅锌矿的热水沉积岩及找矿潜力

经过对黄石板铅锌矿含矿层展布、产态、矿化富集规律等基本特征的总结,以及对含矿层中典型热水沉积岩岩石学特征、岩石化学特征、含矿物质来源初步分析,通过热水沉积岩和盆地正常水沉积围岩的稀土元素地球化学等与南秦岭泥盆纪热水沉积岩的对比、研究,初步认为白河县黄石板铅锌矿为一较典型的热水沉积矿床。提出黄石板矿区西段高家沟一带深部仍存在隐伏矿体的可能性较大,并通过钻探验证发现较富隐伏铅锌矿体。运用热水沉积成岩成矿理论指出该地区找矿方向。     

井地直流电法三维数值模拟中若干问题研究

讨论了地下垂直线源分段计算和场叠加的方法,并实现了在套管上供直流电的三维数值模拟。讨论了大型容量矩阵的压缩存储方式,采用数组和结构体相结合的方法实现容量矩阵的一维链表式压缩存储。在求解超大型稀疏线形方程组时引入不完全Cholesky分解稳定化的双共轭梯度算法(ICBG),通过与均匀半空间垂直线源解析解的对比,证明了该算法是准确可靠的。     

内蒙西部银根-额济纳中生代盆地群叠置类型与勘探领域

内蒙西部银根-额济纳盆地群是在前古生代基底上发育起来的中、新生代“叠置型”盆地群。构造演化经历了三叠纪的热拱隆张阶段、早中侏罗世的初始裂谷盆地阶段、早白垩世的裂谷盆地发育阶段、晚白垩世的引张坳陷阶段、第三纪到第四纪的陆内聚敛挤压阶段。主要形成了下白垩统半深湖相烃源岩,其次为中下侏罗统煤系烃源岩。根据构造层之间的叠置关系,可划分为完全叠置型、基本叠置型、迁移叠置型3种盆地(凹陷)类型。不同叠置类型盆地(凹陷)的烃源岩发育特征、各类圈闭发育特征不同,油气成藏条件差别较大,勘探方向和勘探领域不同。根据裂谷小湖盆的沉积发育特征,应围绕沉积“洼槽”中心的烃源岩开展近源勘探,分别指出了不同叠置型盆地(凹陷)的勘探领域:叠置型盆地(凹陷)主要以控盆断裂带的滚动背斜、缓坡带的岩性、地层不整合圈闭为主要勘探领域;基本叠置型盆地(凹陷)主要以中央断裂隆起构造带的断鼻、断块圈闭为主要勘探领域;迁移叠置型盆地(凹陷)主要以不整合圈闭和缓坡带的岩性圈闭为主要勘探领域。