鄂尔多斯盆地北部苏里格庙含油气区上古生界层序地层研究

在区域构造变动、岩性组合、沉积相构成、测井曲线特征等研究基础上,利用层序地层学原理,对苏里格庙地区上古生界层序地层进行了研究.将在苏里格庙含油气区上古生界划分出5个层序组,并在晋祠组到石盒子组中划分出14个三级沉积层序,分别发育于陆表海、三角洲、河流3种沉积背景之下.建立层序地层格架,以体系域为单位探讨了层序地层格架内主要含气层段-层序8、9的砂体展布规律.研究表明,以体系域为单位编制的砂体等值线图,更细致地刻画了砂体的展布,砂质储集体的发育和空间展布受控于沉积环境,主要发育在低位体系域中.     

准噶尔盆地西北缘扇体形成演化与扇体油气藏勘探

准噶尔盆地西北缘广泛发育二叠纪-侏罗纪冲积扇、水下扇、扇三角洲等砾质粗碎屑沉积,其形成演化严格受不同时期活动的同生断裂控制.二叠纪以乌尔禾组扇体最为发育,呈由盆缘向盆地方向逐渐增强的前展式推覆冲断及渐进式扇体迁移响应模式.三叠纪-侏罗纪以百口泉组、克拉玛依组扇体最为发育,呈由盆内向盆缘方向逐渐减弱的退覆式冲断活动及后退式扇体迁移响应模式.已知扇体油气藏主要富集于水下扇扇根及扇中、扇三角洲平原及前缘4个亚相带,及二叠系佳木河组、乌尔禾组、三叠系百口泉组、克拉玛依组、侏罗系八道湾组、头屯河组6个层位.二叠-三叠纪扇体含油层多、规模大、储量丰度高,侏罗纪扇体反之.受断裂、不整合、岩相岩性、物性4种因素控制,扇体主要形成断块、地层不整合及构造岩性油气藏.断阶带及扇根-扇中相带主要发育构造(断块)油藏,为扇体与断层相配置的垂向运聚成藏模式;斜坡区及扇中-扇缘相带主要发育岩性油藏,为扇体与不整合相配置的侧向运聚成藏模式.西北缘扇体成藏条件好,探明程度总体较低,剩余资源潜力大,进而指出了七大有利勘探区块和方向.     

伊-陕斜坡山2段包裹体古流体势恢复及天然气聚集条件

恢复自烃类生成以来的各个地史时期的古流体势, 有助于正确认识油气藏的分布规律.通过对鄂尔多斯盆地伊-陕斜坡太原组—山西组砂岩储层流体包裹体样品的系统分析, 将其油气充注划分为6个期次; 结合埋藏史分析, 确定出6期油气充注发生的时间.在此基础上, 运用流体包裹体pVT热动力学模拟的方法, 获得了6期油气充注的古压力数据, 并计算出伊-陕斜坡山2段6期次天然气充注的古气势, 分析了古气势分布及时空演化规律, 认为区域构造和热史演化是其主要控制因素.结合区域地质资料, 探讨了天然气运移与聚集规律: 晚三叠世中期至中侏罗世末期, 山2段储层气势西南高而北部、东北部低, 天然气主要从西南向北、东北向运移; 中侏罗世末期至早白垩世末期, 气势西高东低, 天然气主要由西向东就近运移, 再向北和东北向运移; 早白垩世末至现今, 天然气藏进入聚集与散失的动平衡状态, 形成现今分布特征.榆林及其南部地区是天然气聚集的最有利地带, 其次为神木-米脂地区.      

南海北部陆缘新生代玄武岩地球化学特征及成因

南海盆地及周缘地区新生代玄武岩对揭示南海盆地的演化历史至关重要,然而这些玄武岩的成因还存在争议。本文研究了位于南海北部陆缘的海南岛临高县多文组玄武岩岩石地球化学和矿物地球化学特征,并探讨其成因和构造背景。多文组玄武岩主要由橄榄石、单斜辉石、斜长石、斜方辉石、铬尖晶石和铁钛氧化物等组成。橄榄石Fo值变化于55.5～71.1之间,Ni的含量较低,Fe/Mn比值较高。铬尖晶石Cr^#值为74.1～82.7,Mg^#值为45.5～63.8, Ti的含量较高。斜方辉石Mg^#值为63.9～79.6,单斜辉石为66.0～80.6。单斜辉石稀土配分曲线富集MREE,亏损LREE和HREE,呈拱形分布。斜长石以中-拉长石为主(Ab_{36.56～52.78}),富集LREE、Ba、Sr和Eu。铁钛氧化物的TiO₂含量为50.19%～51.46%。多文组玄武岩原始岩浆的主量和微量元素组成与夏威夷、峨眉山、塔里木等玄武岩组成一致,地幔源区包含了辉石岩的成分,而且其地幔潜在温度(>1400℃)和氧逸度(Δ...     

鄂尔多斯盆地天环坳陷北段奥陶系烃源岩特征及成熟演化史

为研究天环坳陷北段下古生界天然气成藏规律,利用探井资料和有机地球化学方法,评价了天环坳陷北段奥陶系烃源岩特征并恢复其成熟演化史。天环坳陷北段奥陶系乌拉力克组和克里摩里组烃源岩有机碳含量和生烃潜量相对较高,烃源岩有机质丰度以中等—好为主,少部分为差烃源岩;三道坎组和桌子山组烃源岩以差为主。干酪根组分鉴定表明,天环坳陷北段奥陶系烃源岩主要为Ⅱ₁～Ⅰ型干酪根,热演化程度高,处于生干气阶段。成熟演化史模拟显示,古生代—中生代早期地温梯度低,地层埋藏浅,烃源岩成熟演化程度低。燕山期,由于构造热事件,地温梯度迅速升高,早白垩世烃源岩经历的最高温度超过200℃,达到生气高峰期,早白垩世是油气成藏的主要时期。早白垩世之后,鄂尔多斯盆地整体抬升,地温梯度减小,生烃作用停止。     

河北宣化土城子组恐龙足迹化石新发现

本文报道了新近发现于河北宣化地区土城子组的恐龙足迹化石及沉积环境。为确定足迹化石的地质年代、土城子组的沉积环境及足迹化石属种,本文在对恐龙足迹化石层及其上、下地层进行剖面测制、沉积相划分和沉积环境分析的基础上,对化石层上覆凝灰岩层进行了LA-ICPMS锆石U-Pb测年,并对保存较好的足迹化石进行了测量和对比研究工作。研究结果表明,土城子组底部为冲积扇扇中沉积环境,足迹化石上、下地层则表现为河流相沉积环境,而足迹化石的赋存层位形成于滨湖相沉积环境,发育暴露构造并含有大量裸子植物碎屑化石。凝灰岩锆石U-Pb加权平均年龄为152.3±0.3 Ma(MSWD=0.00106),说明化石层位于土城子组一段,时代属于晚侏罗世钦莫利期(Kimmeridgian)中晚期。已发现的足迹化石以兽脚类三趾型足迹为主,包括跷脚龙足迹属(Grallator)、安琪龙足迹属(Anchisauripus)和实雷龙足迹属(Eubrontes),其次为一些疑似蜥脚类恐龙足迹,是华北北缘土城子组中群落丰富度最高的恐龙足迹点,其中一处或许为中国北方面积最大的恐龙足迹点。因此,我们认为宣化-下花园盆地土城子组一段以河流、湖泊...     

钦防海西-印支海槽西界断裂新探

本文主要根据二维地震剖面并结合野外露头的分析认为,十万大山盆地东南缘的基底断裂是钦防海槽向北西冲断-推覆的前锋断层,断裂两侧的中、古生界在地层层位与厚度上存在明显差异。钦防海西-印支海槽的西界不应是灵山断裂,而应是十万大山盆地东南缘的基底断裂,其范围远大于现今博(白)—罗(定)—广(宁)断裂与灵山断裂之间的范围。基底断裂为一无根的推覆构造带,其下掩覆了十万大山盆地东南缘的许多区域,是下一步油气勘探的重要领域。     

Impacts of Aerosol-Radiation Interactions on the Wintertime Particulate Pollution under Different Synoptic Patterns in the Guanzhong Basin,China

The effects of aerosol–radiation interactions(ARI) are not only important for regional and global climate, but they can also drive particulate matter(PM) pollution. In this study, the ARI contribution to the near-surface fine PM(PM2.5)concentrations in the Guanzhong Basin(GZB) is evaluated under four unfavorable synoptic patterns, including "northlow", "transition", "southeast-trough", and "inland-high", based on WRF-Chem model simulations of a persistent heavy PM pollution episode in January 2019. Simulations show that ARI consistently decreases both solar radiation reaching down to the surface(SWDOWN) and surface temperature(TSFC), which then reduces wind speed, induces sinking motion,and influences cloud formation in the GZB. However, large differences under the four synoptic patterns still exist. The average reductions of SWDOWN and daytime TSFC in the GZB range from 15.2% and 1.04°C in the case of the"transition" pattern to 26.7% and 1.69°C in the case of the "north-low" pattern, respectively. Furthermore, ARI suppresses the development of the planetary boundary layer(PBL), with the decrease of PBL height(PBLH) varying from 18.7% in the case of the "transition" pattern to 32.0% in the case of the "north-low" pattern. The increase of daytime near-surface PM2.5 in the GZB due to ARI is 12.0%, 8.1%, 9.5%, and 9.7% under the four synoptic patterns, respectively. Ensemble analyses also reveal that when near-surface PM2.5 concentrations are low, ARI tends to lower PM2.5 concentrations with decreased PBLH, which is caused by enhanced divergence or a transition from divergence to convergence in an area. ARI contributes 15%–25% toward the near-surface PM2.5 concentrations during the severe PM pollution period under the four synoptic patterns.     

A constitutive model for mechanical and chemo‐mechanical compaction in sedimentary basins and finite element analysis

Compaction and associated fluid flow are fundamental processes in sedimentary basin deformation. Purely mechanical compaction originates mainly from pore fluid expulsion and rearrangement of solid particles during burial, while chemo‐mechanical compaction results from Intergranular Pressure‐Solution (IPS) and represents a major mechanism of deformation in sedimentary basins during diagenesis. The aim of the present contribution is to provide a comprehensive 3D framework for constitutive and numerical modeling of purely mechanical and chemo‐mechanical compaction in sedimentary basins. Extending the concepts that have been previously proposed for the modeling of purely mechanical compaction in finite poroplasticity, deformation by IPS is addressed herein by means of additional viscoplastic terms in the state equations of the porous material. The finite element model integrates the poroplastic and poroviscoplastic components of deformation at large strains. The corresponding implementation allows for numerical simulation of sediments accretion/erosion periods by progressive activation/deactivation of the gravity forces within a fictitious closed material system. Validation of the numerical approach is assessed by means of comparison with closed‐form solutions derived in the context of a simplified compaction model. The last part of the paper presents the results of numerical basin simulation performed in one dimensional setting, demonstrating the ability of the modeling to capture the main features in elastoplastic and viscoplastic compaction. Copyright © 2016 John Wiley & Sons, Ltd.