Sequence Stratigraphy of the Lower Cretaceous Uraniferous Measures and Mineralization of the Sandstone-hosted Tamusu Large Uranium Deposit, North China

The Bayingobi basin is the Mesozoic-Cenozoic basin in North China in which the Tamusu uranium deposit is located.The ore-target layer of the deposit is the Lower Cretaceous Bayingobi Formation,which developed as a fan deltashallow lacustrine deposit.The distributary channel sand body of the fan delta plain and the underwater distributary channel sand body of the fan delta front formed a favorable uranium reservoir,so the study of sequence stratigraphy is extremely important to understanding the genesis of uranium deposits.On the basis of field investigation and a large number of borehole logs,the high resolution sequence stratigraphy of the Lower Cretaceous is divided and the system tracts of different periods are established.The relationship between deposition,interlayer oxidation and uranium enrichment is discussed.The Lower Cretaceous Bayingobi Formation can be divided into two fourth-order sequences(Sq1 and Sq2).The lower member of the Bayingobi Formation is referred to as Sq1,which is composed of a falling-stage system tract(FSST)on top.On the other hand,the upper member of the Bayingobi Formation is referred to as Sq2,which is composed of a lowstand system tract(LST),transgressive system tract(TST)and highstand system tract(HST).The lowstand system tract forms a favorable stratigraphic structure(mud-sand-mud formation)with the lacustrine mudstone of the overlying transgressive system tract,that is conducive for the migration of uranium-bearing oxygen water.The organic matter and pyrite in the fan delta sand body,as well as the dark mudstone in the distributary bay,provided a reducing medium for uranium mineralization.The ore body mainly occurs in the distributary channel,underwater distributary channel or the mouth bar of the fan delta.As a result of the moderate thickness,high permeability,favorable barrier and rich reducing medium,the rich ore body mainly occurs in the underwater distributary channel and mouth bar sand body of the delta front.Based on study of the sequence stratigraphy,the model of the sequence,sedimentation and mineralization of the uranium deposit is established,which enriches uranium metallogenic theory and provides a reference for exploration of the same type of uranium deposits.     

珠Ⅰ坳陷油源对比及恩平组烃源岩的相对贡献

恩平组烃源岩成藏贡献研究对于拓展珠Ⅰ坳陷勘探新领域以及发现新的储量具有重要的应用价值, 目前相关研究较少.在油源对比的基础上, 将生标绝对含量与端元油配比实验相结合, 研究了珠Ⅰ坳陷恩平组烃源岩对单井油样的相对贡献.油源对比结果指示, 研究区原油可分为3类: 第1类源自始新统文昌组中深湖相烃源岩, 主要分布在惠陆低凸起、番禺4洼、流花凸起等地区; 第2类源自始新统-渐新统恩平组湖沼相烃源岩, 仅分布在惠州凹陷北部; 第3类为混源油, 发现于惠州凹陷南部和恩平凹陷.甾萜类绝对含量等7个指标建立的混源比例图版适用于计算油样中前两类烃源岩的相对贡献.计算结果表明, 文昌组烃源岩是珠Ⅰ坳陷的主力烃源岩, 恩平组烃源岩仅对惠州凹陷和恩平凹陷中的部分油样存在贡献.      

Critical Controlling Factors of Shale Gas Enrichment and Accumulation, and Remaining Uncertainties

<正>Shale gas exploration have yielded remarkable achievements recently in China,and four national demonstration areas for shale gas exploration and production have been established respectively as FulingJiaoshiba,Changning-Weiyuan,Zhaotong and Yanchang.During recent few years,nearly 400 wells have been drilled including 143 exploratory wells(vertical wells)and     

南京汤山温泉区地热水成因模式分析

汤山温泉是中国四大著名温泉疗养胜地之一,阐明其成因模式对于该温泉区的进一步开发和热水资源的可持续利用具有一定意义。基于硅-焓图解法和水文地球化学方法对其进行了系统研究,结果表明该区热储温度为90℃,岩溶热水与岩溶冷水、孔隙潜水和地表水之间在水化学和同位素组成上存在明显差异,地热井深度越大,冷水混入相对较少,地热水温度相对较高。经分析,该地热系统成因上属于中低温对流型。其补给区主要来自汤山山体(宁镇山区)及句容盆地东侧茅山山脉,循环深度为2.6~2.9 km,地热水通过汤山-东昌街断裂在浅部与区内NW向断裂、NE向断裂交汇形成温泉水。     

1953～2017年黄河源区气温变化的多尺度特征

基于黄河源区8个站点的年平均气温序列,利用集合经验模态分解（Ensemble Empirical Mode Decomposition,EEMD）方法,揭示了以玛多站为代表的黄河源区1953~2017年气温演变的多时间尺度特征,探讨不同时间尺度上的周期振荡对气温变化总体特征的影响程度,分析了黄河源区不同时间尺度的气温变化与海温指数,尤其是与北大西洋多年代际振荡（Atlantic Multidecadal Oscillation,AMO）间的关系。结果表明:（1）1953年以来黄河源区玛多站年平均气温以0.31 ℃/10 a的变化率表现为明显的增暖趋势,20世纪80年代后期开始转暖,尤其是进入20世纪90年代后期变暖更加明显。（2）1953~2017年,黄河源区年平均气温呈现3 a、6 a、11 a、25 a、64 a及65 a以上时间尺度的准周期变化,其中以准3 a和65 a以上时间尺度的振荡最显著,准3 a的年际振荡在21世纪以前振幅较大,而进入21世纪后年际振荡振幅减弱,65 a以上时间尺度的年代际振荡振幅明显加大。（3）1998年气候显著变暖以前,以准3 a周期为代表的年际振荡在气温演变过程中占据主导地位,1998年气候显著变暖以后,65 a以上时间尺度周期振荡的贡献率增加近5倍,与准3 a周期振荡的贡献相当。（4）气温与Nino3.4指数和PDO（Pacific Decadal Oscillation）指数的同期相关均不显著,但当气温领先PDO指数22 a时正相关最大且显著,不同于PDO指数,气温原始序列及其3个年代际尺度分量滞后AMO指数3~7 a或二者同期时相关性最高,这就意味着AMO对黄河源区气温具有显著影响。（5）AMO的正暖位相对应着包括中国的整个东亚地区偏暖,黄河源区只是受影响区域的一部分,20世纪60年代至90年代初期AMO的负冷位相期、20世纪90年代中后期至今AMO的正暖位相与黄河源区气温距平序列的负距平、正距平相对应,气温在65 a以上时间尺度的变化与AMO指数相关性更高,可见,AMO是影响黄河源区气温变化的一个重要的气候振荡,这种影响主要表现在年代际时间尺度上。     

Long-term Stability and Oceanic Mean State Simulated by the Coupled Model FGOALS-s2

We describe the long-term stability and mean climatology of oceanic circulations simulated by version 2 of the Flexible Global Ocean-Atmosphere-Land System model(FGOALS-s2).Driven by pre-industrial forcing,the integration of FGOALS-s2 was found to have remained stable,with no obvious climate drift over 600 model years.The linear trends of sea SST and sea surface salinity(SSS) were 0.04°C(100yr)-1 and 0.01 psu(100yr)-1,respectively.The simulations of oceanic temperatures,wind-driven circulation and thermohaline circulation in FGOALS-s2 were found to be comparable with observations,and have been substantially improved over previous FGOALS-s versions(1.0 and 1.1).However,significant SST biases(exceeding 3°C) were found around strong western boundary currents,in the East China Sea,the Sea of Japan and the Barents Sea.Along the eastern coasts in the Pacific and Atlantic Ocean,a warm bias(>3°C) was mainly due to overestimation of net surface shortwave radiation and weak oceanic upwelling.The difference of SST biases in the North Atlantic and Pacific was partly due to the errors of meridional heat transport.For SSS,biases exceeding 1.5 psu were located in the Arctic Ocean and around the Gulf Stream.In the tropics,freshwater biases dominated and were mainly caused by the excess of precipitation.Regarding the vertical dimension,the maximal biases of temperature and salinity were located north of 65°N at depths of greater than 600 m,and their values exceeded 4°C and 2 psu,respectively.     

Oceanic climatology in the coupled model FGOALS-g2: Improvements and biases

The present study examines simulated oceanic climatology in the Flexible Global Ocean-Atmosphere-Land System model, Grid-point Version 2 (FGOALS-g2) forced by historical external forcing data. The oceanic temperatures and circulations in FGOALS-g2 were found to be comparable to those observed, and substantially improved compared to those simulated by the previous version, FGOALS-g1.0. Compared with simulations by FGOALS-g1.0, the shallow mixed layer depths were better captured in the eastern Atlantic and Pacific Ocean in FGOALS-g2. In the high latitudes of the Northern Hemisphere, the cold biases of SST were about 1°C–5°C smaller in FGOALS-g2. The associated sea ice distributions and their seasonal cycles were more realistic in FGOALS-g2. The pattern of Atlantic Meridional Overturning Circulation (AMOC) was better simulated in FGOALS-g2, although its magnitude was larger than that found in observed data. The simulated Antarctic Circumpolar Current (ACC) transport was about 140 Sv through the Drake Passage, which is close to that observed. Moreover, Antarctic Intermediate Water (AAIW) was better captured in FGOALS-g2. However, large SST cold biases (>3°C) were still found to exist around major western boundary currents and in the Barents Sea, which can be explained by excessively strong oceanic cold advection and unresolved processes owing to the coarse resolution. In the Indo-Pacific warm pool, the cold biases were partly related to the excessive loss of heat from the ocean. Along the eastern coast in the Atlantic and Pacific Oceans, the warm biases were due to overestimation of shortwave radiation. In the Indian Ocean and Southern Ocean, the surface fresh biases were mainly due to the biases of precipitation. In the tropical Pacific Ocean, the surface fresh biases (>2 psu) were mainly caused by excessive precipitation and oceanic advection. In the Indo-Pacific Ocean, fresh biases were also found to dominate in the upper 1000 m, except in the northeastern Indian Ocean. There were warm and salty biases (3°C–4°C and 1–2 psu) from the surface to the bottom in the Labrador Sea, which might be due to large amounts of heat transport and excessive evaporation, respectively. For vertical structures, the maximal biases of temperature and salinity were found to be located at depths of >600 m in the Arctic Ocean, and their values exceeded 4°C and 2 psu, respectively.     

东营市东营区努力开创国土资源信访工作新局面

近年来，东营区国土资源局不断加大信访宣传工作力度，强化信访工作责任，完善信访管理机制，全面提高基层信访工作水平，使信访工作重心和责任下移，努力从源头上减少信访问题的发生。连续3年荣获“全省国土资源信访工作先进单位”荣誉称号。     

青藏高原多年冻土概论

本文较系统地阐述了青藏高原多年冻土的地带性规律、冻土构造以及融区的类型和分布特征,详细论述了不同作用下形成的冻土(冰缘)地貌,并对青藏高原的冰缘期进行了初步划分与对比。     

东太平洋冷舌区海表面温度日变化特征的模拟研究

本文通过分辨太阳辐射日变化, 利用中国科学院大气物理研究所大气科学和地球流体力学数值模拟国家重点实验室 (LASG/IAP) 气候系统海洋环流模式 (LICOM), 模拟了东太平洋冷舌区海表面温度 (SST) 的日变化特征并研究了弱混合对其影响。采用理想的太阳辐射日变化强迫上层垂向分辨率为10 m的海洋模式LICOM, 模拟出了SST日变化一些特征, 同时海洋的上层流场也产生明显日变化。模拟的SST日变化振幅水平分布与观测接近, 且受太阳辐射日变化振幅水平分布调制。在赤道中东太平洋区, 模拟的SST日变化振幅 (约为0.3～0.4℃) 比观测偏小约0.1～0.2℃。模拟的SST日变化峰值出现在15～16 时 (当地标准时间), 落后于太阳辐射峰值2～3个小时, 接近观测。进一步减弱混合后, 模拟的日变化振幅增加约0.1℃, 更接近观测。这说明在东太平洋冷舌区SST日变化主要受太阳辐射日变化和垂直混合影响。此外, 混合减小后, 在太阳辐射日变化调制下, 平均态 (如混合层、温度和流场) 也出现明显变化。在赤道东太平洋冷舌区北侧, 弱混合导致混合层变浅, 变浅使热量堆积进而使平均SST升高约0.3℃; 在赤道东太平洋冷舌南侧, 经向平流加强导致平均SST降低约0.2℃。