河南省嵩山区元古代嵩山群底部的主滑脱带          下载免费PDF全文

索书田  游振东  闻立峰  韩郁菁 《地球科学》2019,44(5):1537-1543

河南省嵩山区位于中朝地台南部,区内发育被2个角度不整合面分隔开的3个前寒武纪岩群,一个主滑脱带沿着嵩山群与登封群间不整合面发育.滑脱带之上的早元古代嵩山群形成近南北向的褶皱带,因此,嵩山群岩石在主滑脱带之上形成无根的独立构造.与滑脱带下伏的太古宙登封群很少有关系.主滑脱带厚4～30m,沿着主滑脱带,登封群角闪岩相岩石强烈退变质到绿片岩相矿物组合,主滑脱带发育在脆韧性过渡域.多尺度的观察指出,主滑脱带的形成受地壳成分分层导致的流变学分层性所制约,而且地层柱底部软弱面或地质界面是近水平的滑脱带发育的优选位置.显然,对滑脱带的发育还必须考虑水解弱化作用.  相似文献   

水平分层胶结充填体损伤本构模型及强度准则     

汪杰  宋卫东  谭玉叶  付建新  曹帅 《岩土力学》2019,40(5):1731-1739

以矿山分层充填为背景,针对水平分层充填体,提出了初始分层损伤、荷载损伤与总损伤的概念;利用损伤力学理论,考虑分层效应,建立了充填体损伤演化及本构模型;基于全微分方法构建了考虑分层效应的充填体强度准则。开展了不同分层充填体力学特性试验。研究结果表明：所建立的分层充填体损伤本构模型及强度准则理论曲线与试验曲线高度吻合,验证了模型的正确性;初始分层损伤随分层数增多,呈现 的二次多项式递增,分层效应与荷载耦合作用劣化了充填体总损伤;充填体总损伤率呈先增大后减小趋势。在峰值之前,分层数越多,则总损伤率越大;而峰值之后,分层数越多,则总损伤率越小,且总损伤率最大值随分层数增多而增大。  相似文献   

Alluvial stratification styles in a large,flash‐flood influenced dryland river: The Luni River,Thar Desert,north‐west India     

Paul A. Carling  Suzanne F. Leclair 《Sedimentology》2019,66(1):102-128

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Another Year of Record Heat for the Oceans     

Lijing CHENG  John ABRAHAM  Kevin E.TRENBERTH  John FASULLO  Tim BOYER  Michael E.MANN  Jiang ZHU  Fan WANG  Ricardo LOCARNINI  Yuanlong LI  Bin ZHANG  Fujiang YU  Liying WAN  Xingrong CHEN  Licheng Feng  Xiangzhou SONG  Yulong LIU  Franco RESEGHETTI  Simona SIMONCELLI  Viktor GOURETSKI  Gengxin CHEN  Alexey MISHONOV  Jim REAGAN  Guancheng LI 《大气科学进展》2023,40(6):963-974

Changes in ocean heat content(OHC), salinity, and stratification provide critical indicators for changes in Earth’s energy and water cycles. These cycles have been profoundly altered due to the emission of greenhouse gasses and other anthropogenic substances by human activities, driving pervasive changes in Earth’s climate system. In 2022, the world’s oceans, as given by OHC, were again the hottest in the historical record and exceeded the previous 2021 record maximum.According to IAP/CAS data, ...  相似文献   

A LIMITED-LENGTH-SCALE k-ε MODEL FOR THE NEUTRAL AND STABLY-STRATIFIED ATMOSPHERIC BOUNDARY LAYER     

DAVID D. APSLEY  IAN P. CASTRO 《Boundary-Layer Meteorology》1997,83(1):75-98

Analytical and numerical models of the neutral and stably-stratifiedatmospheric boundary layer are reviewed. Theoretical arguments andcomputational models suggest that a quasi-steady state is attainable in aboundary layer cooled from below and it is shown how this may be incorporatedwithin a time-steady, one-dimensional model. A new length-scale-limitedk- model is proposed for flows where a global maximum mixing length isimposed by the finite boundary-layer depth or, in stably-stratifiedconditions, by the Obukhov length, whilst still reducing to a form consistentwith the logarithmic law in the surface layer. Simulations compare favourablywith data from the Leipzig experiment and from Cardington airfield inEngland.  相似文献   

TURBULENCE STRUCTURE IN A STRATIFIED BOUNDARY LAYER UNDER STABLE CONDITIONS   总被引：2，自引：2，他引：0  

YUJI OHYA  DAVID E. NEFF  ROBERT N. MERONEY 《Boundary-Layer Meteorology》1997,83(1):139-162

Turbulence structure in stably stratified boundary layers isexperimentally investigated by using a thermally stratified wind tunnel. Astably stratified flow is created by heating the wind tunnel airflow to atemperature of about 50 °C and by cooling the test-section floor to asurface temperature of about 3 °C. In order to study the effect ofbuoyancy on turbulent boundary layers for a wide range of stability, thevelocity and temperature fluctuations are measured simultaneously at adownwind position of 23.5 m from the tunnel entrance, where the boundarylayer is fully developed. The Reynolds number, Re, ranges from 3.14× 104 to 1.27 × 105, and the bulk Richardson number, Ri,ranges from 0 to 1.33. Stable stratification rapidly suppresses thefluctuations of streamwise velocity and temperature as well as the verticalvelocity fluctuation. Momentum and heat fluxes are also significantlydecreased with increasing stability and become nearly zero in the lowest partof the boundary layer with strong stability. The vertical profiles ofturbulence quantities exhibit different behaviour in three distinct stabilityregimes, the neutral flows, the stratified flows with weak stability(Ri = 0.12, 0.20) and those with strong stability (Ri= 0.39,0.47, 1.33). Of these, the two regimes of stratified flows clearly showdifferent vertical profiles of the local gradient Richardson number Ri,separated by the critical Richardson number Ri cr of about 0.25. Moreover,turbulence quantities in stable conditions are well correlated with Ri.  相似文献   

The forming-storing environment and abundance conditions of quaternary underground brine in the embayed coast of Qingdao     

韩有松  王少青  孟广兰 《中国海洋湖沼学报》1997,15(4):332-341

ImODUcrIONGroundwaterwthAnneralimtionofmorethan5OgA(about5"Be')"iscalledunder-groundbrine.ltbelongstoevaporationoredepositinliquidstateandisantwortantrnaterialsourceforsaltonkingandthechewhcalindustry.QuatemarylittoralfadesundergroundbrinewasstoredinthelittoralsoneandhadtwobasictypesofgenesisenvironmentflittoralplaincoastenvironmentcharacterindbythecoastalongLaichouBay,andembayedcoastenvironmentcharaCterindbythecoastalzoneofQingdao.TheauthorresearchedthebrineintheLaizhoubaycoastareainthe…  相似文献   

柴达木盆地盐湖锂矿床成矿过程及分布规律   总被引：2，自引：1，他引：1  

余俊清  洪荣昌  高春亮  成艾颖  张丽莎 《盐湖研究》2018,26(1):7-14

柴达木盆地盐湖蕴藏230×10~4t锂,集中分布在别勒滩、东西台等4个盐湖,占我国卤水锂资源总量~80%,战略资源地位不言而喻。近年来提锂技术及工程化研究倍受重视,而对盐湖锂矿成因和分布规律的了解凸显不足,锂矿资源流失严重与之不无关联。研究查明,昆仑山高温热泉群含锂泉水长期注入洪—那河,流入终端盐湖,蒸发富集成矿;锂的年输入通量748.8 t,结合区内盐湖锂矿总储量保守估算,成矿期始于14 ka BP之后;洪—那河早期主要流向别勒滩,在山前冲积扇向北推进、扇前河改道北流后,方才形成含锂河水当前分配格局。据此,破解了别勒滩锂矿在研究区储量最大的原由。还查明了锂矿床仅存在于别勒滩,而在达布逊等3个区段不能成矿的原因。阐明了锂的来源与新生代火山喷发岩、深部岩浆房、昆仑大断裂活动有关,以及含锂热水持续远程输送至盐湖成矿的地貌和水文气候动因。企业应当根据锂的分布规律和矿床特征,迅速转变钾肥生产模式。  相似文献   

岩土勘察与盐湖卤水矿产开发          下载免费PDF全文

颜辉 《盐湖研究》2018,26(4):85-90

通过对盐湖地区岩土类型复杂性及特性的叙述,分析了盐湖矿产开发中不良地质现象产生的原因和岩土条件对开发规模、工程布局、工程安全、经济效益等方面产生的影响。论述岩土工程勘察在盐湖矿产开发中的特殊地位和重要价值,总结出岩土勘察与盐湖卤水矿产开发的关系,提出盐湖岩土勘察方案的相关建议。  相似文献   

察尔汗盐湖察尔汗二级补给系统S3盐层晶间卤水中KCl的分异特征、富集规律及其成因   总被引：1，自引：0，他引：1       下载免费PDF全文

徐少康 《盐湖研究》1999,7(1):1

据ＫＣｌ含量的概率分布特征,晶间卤水分为７个总体。晶间卤水ＫＣｌ,在三级系统内水平分异有２种、剖面分异有５种,二级系统内水平分异呈环带状、剖面分异形式为三级系统内分异形式的组合,垂直分异有１３种;富集的总体为Ⅳ（ｋｃｌ）、Ⅲ（ｋｃｌ）用Ｖ（ｋｃｌ）、三级系统为（８）和（１０）号、部位为固相钾高含处;分异及富集的成因主要为晶间卤水的阶段性淡化。  相似文献