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Fault zone structures of northern and southern portions of the main central fault generated by the 2008 Wenchuan earthquake using fault zone trapped waves 被引量:16
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作者 Songlin Li Xiaoling Lai +1 位作者 Zhixiang Yao Qing Yang 《Earthquake Science》 CSCD 2009年第4期417-424,共8页
The rupture process of the May 12, 2008 Ms8.0 Wenchuan earthquake was very complex. To study the rupture zones generated by this earthquake, four dense temporary seismic arrays across the two surface breaking traces o... The rupture process of the May 12, 2008 Ms8.0 Wenchuan earthquake was very complex. To study the rupture zones generated by this earthquake, four dense temporary seismic arrays across the two surface breaking traces of the main-shock were deployed in July and recorded a great amount of aftershocks. This paper focuses on the data interpretation of two arrays across the central main fault, the northern array line 1 and southern array line 3. The fault zone trapped waves recorded by the two arrays were used to study the structure of the central main fault and the difference between the northern and southern portions. The results show that the widths of the rupture zone are about 170-200 m and 200-230 m for northern and southern portions respectively. And the corresponding dip angles are 80° and 70°. The seismic velocity inside the fracture zone is about one half of the host rock. By comparison, the northern portion of the rupture zone is slightly narrower and steeper than the southern portion. Besides these differences, one more interesting and important difference is the positions of the rupture zone with respect to surface breaking traces. At the northern portion, the rupture zone is centered at the surface breaking trace, while at the southern portion it is not but is shifted to the northwest. This difference reflects the difference of rupture behaviors between two portions of the central main fault. The width of the rupture zone is smaller than that of MS.1 Kunlun earthquake though these two earthquakes have almost the same magnitudes. Multiple ruptures may be one factor to cause the narrower rupture zone. 展开更多
关键词 Wenchuan earthquake seismic rupture zone fault zone trapped waves
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Rock Damage Structure of the South Longmen-Shan Fault in the 2008 M8 Wenchuan Earthquake Viewed with Fault-Zone Trapped Waves and Scientific Drilling 被引量:9
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作者 LI Yonggang XU Zhiqin LI Haibing 《Acta Geologica Sinica(English Edition)》 SCIE CAS CSCD 2014年第2期444-467,共24页
This article is to review results from scientific drilling and fault-zone trapped waves (FZTWs) at the south Longman-Shan fault (LSF) zone that ruptured in the 2008 May 12 M8 Wenchuan earthquake in Sichuan,China.I... This article is to review results from scientific drilling and fault-zone trapped waves (FZTWs) at the south Longman-Shan fault (LSF) zone that ruptured in the 2008 May 12 M8 Wenchuan earthquake in Sichuan,China.Immediately after the mainshock,two Wenchuan Fault Scientific Drilling (WFSD) boreholes were drilled at WFSD-1 and WFSD-2 sites approximately 400 m and 1 km west of the surface rupture along the Yinxiu-Beichuan fault (YBF),the middle fault strand of the south LSF zone.Two boreholes met the principal slip of Wenchuan earthquake along the YBF at depths of 589-m and 1230-m,respectively.The slip is accompanied with a 100-200-m-wide zone consisting of fault gouge,breccia,cataclasite and fractures.Close to WFSD-1 site,the nearly-vertical slip of ~4.3-m with a 190-m wide zone of highly fractured rocks restricted to the hanging wall of the YBF was found at the ground surface after the Wenchuan earthquake.A dense linear seismic array was deployed across the surface rupture at this venue to record FZTWs generated by aftershocks.Observations and 3-D finite-difference simulations of FZTWs recorded at this cross-fault array and network stations close to the YBF show a distinct low-velocity zone composed by severely damaged rocks along the south LSF at seismogenic depths.The zone is several hundred meters wide along the principal slip,within which seismic velocities are reduced by ~30-55% from wall-rock velocities and with the maximum velocity reduction in the ~200-m-wide rupture core zone at shallow depth.The FZTW-inferred geometry and physical properties of the south LSF rupture zone at shallow depth are in general consistent with the results from petrological and structural analyses of cores and well log at WFSD boreholes.We interpret this remarkable low-velocity zone as being a break-down zone during dynamic rupture in the 2008 M8 earthquake.We examined the FZTWS generated by similar earthquakes before and after the 2008 mainshock and observed that seismic velocities within fault core zone was reduced by ~10% due to severe damage of fault rocks during the M8 mainshock.Scientific drilling and locations of aftershocks generating prominent FZTWs also indicate rupture bifurcation along the YBF and the Anxian-Guangxian fault (AGF),two strands of the south LSF at shallow depth.A combination of seismic,petrologic and geologic study at the south LSF leads to further understand the relationship between the fault-zone structure and rupture dynamics,and the amplification of ground shaking strength along the low-velocity fault zone due to its waveguide effect. 展开更多
关键词 Rupture zone rock damage structure scientific drilling fault-zone trapped waves Wenchuan Earthquake Longmen-Shan Fault
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Fault-zone trapped waves at Muyu in Wenchuan earthquake region 被引量:2
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作者 Lai Xiaoling Sun Yi 《Geodesy and Geodynamics》 2011年第2期66-70,共5页
Trapped waves in the Qingchuan fault zone were observed at Muyu near the northeastern end of the fractured zone of the Wenchuan Ms8. 0 earthquake. The results indicate a fault-zone width of about 200 m and a great dif... Trapped waves in the Qingchuan fault zone were observed at Muyu near the northeastern end of the fractured zone of the Wenchuan Ms8. 0 earthquake. The results indicate a fault-zone width of about 200 m and a great difference in physical property of the crust on different sides of the fault. The inferred location of crustal changes is consistent with land-form boundary on the surface 展开更多
关键词 Wenchuan earthquake region fault-zone trapped waves Longmenshan fault belt seismic records Qingchuan fault
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Fault zone trapped waves at Longmenshan fault belt
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作者 Sun Yi Lai Xiaoling 《Geodesy and Geodynamics》 2013年第3期48-52,共5页
Trapped waves in different sections of Longmenshan fault belt were observed, and the results show the difference between the northern and southern portions of this fault belt. Guanzhuang and Leigu surveying lines are ... Trapped waves in different sections of Longmenshan fault belt were observed, and the results show the difference between the northern and southern portions of this fault belt. Guanzhuang and Leigu surveying lines are located at the northern portion of the fault belt, and the result indicates that the width of the rupture zone underground in this area is about 160 - 180 m. The center position of rupture zone underground corresponds to the surface breaking trace, and is equally distributed at the edges of the two fault walls. However, Hongkou surveying line is located at the southern portion of the fault belt, and the result indicates that the width of the rupture zone underground in this area is about 180 -200 m. The rupture zone underground is mainly distributed below fault scarp. The Wenchuan MsS. 0 earthquake and Lushan Ms7.0 earthquake both occurred at the Longmenshan fault belt. The results will provide information for the structure background of the two violent earthquakes. 展开更多
关键词 Longmenshan fault belt fault zone trapped waves seismic record sectional difference
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Study on rupture zone of the M=8.1 Kunlun Mountain earthquake using fault-zone trapped waves
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作者 李松林 张先康 樊计昌 《Acta Seismologica Sinica(English Edition)》 EI CSCD 2005年第1期43-52,共10页
The observation of the fault-zone trapped waves was conducted using a seismic line with dense receivers across surface rupture zone of the M=8.1 Kunlun Mountain earthquake. The fault zone trapped waves were separated ... The observation of the fault-zone trapped waves was conducted using a seismic line with dense receivers across surface rupture zone of the M=8.1 Kunlun Mountain earthquake. The fault zone trapped waves were separated from seismograms by numerical filtering and spectral analyzing. The results show that: a) Both explosion and earthquake sources can excite fault-zone trapped waves, as long as they locate in or near the fault zone; b) Most energy of the fault-zone trapped waves concentrates in the fault zone and the amplitudes strongly decay with the distance from observation point to the fault zone; c) Dominant frequencies of the fault-zone trapped waves are related to the width of the fault zone and the velocity of the media in it. The wider the fault zone or the lower the velocity is, the lower the dominant frequencies are; d) For fault zone trapped waves, there exist dispersions; e) Based on the fault zone trapped waves observed in Kunlun Mountain Pass region, the width of the rupture plane is deduced to be about 300 m and is greater than that on the surface. 展开更多
关键词 fault-zone trapped waves M=8.1 Kunlun Mountain earthquake seismic rupture plane
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Exploration of fault-zone trapped waves at Pingtong Town,in Wenchuan earthquake region
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作者 Xiaoling Lai Songlin Li Yi Sun 《Geodesy and Geodynamics》 2010年第1期29-33,共5页
Pingtong Town is located on the fractured zone of the Wenchuan 8.0 earthquake, and is seriously damaged by the earthquake. Our observation line is centered at an earthquake exploration trench across the fractured zone... Pingtong Town is located on the fractured zone of the Wenchuan 8.0 earthquake, and is seriously damaged by the earthquake. Our observation line is centered at an earthquake exploration trench across the fractured zone in the NW-SE direction, and is about 400 m long. The results reveal trapped waves in the rup- tured fault zone of the earthquake, and indicate a great difference in physical property between the media inside and outside the fault zone. The predominant frequency of the fault-zone trapped waves is about 3 -4 Hz. The wave amplitudes are larger near the exploration trench. The width of the fault zone in the crust at this location is estimated to be 200 m. In some records, the waveforms and the arrival times of S waves are quite different between the two sides of the trench. The place of change coincides with the boundary of uplift at the surface. 展开更多
关键词 Wenchuan earthquake region fault-zone trapped waves Longmenshan fault belt EXPLORATION seismic records
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SEM Numerical Simulation of Vertical and Inclined Fault Zone Trapped Waves and Comparison of Their Wave Fields
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作者 Xu Hongwei Wang Weijun 《Earthquake Research in China》 CSCD 2015年第2期176-189,共14页
Fault zone trapped waves (FZTWs) mainly travel along the fractured fault zone (FZ) which is of low velocity and high attenuation. FZTWs often carry significant information about a fault's internal structure, so i... Fault zone trapped waves (FZTWs) mainly travel along the fractured fault zone (FZ) which is of low velocity and high attenuation. FZTWs often carry significant information about a fault's internal structure, so it is important to understand their wave field characteristics for FZ structure inversion. Most previous simulations are based on vertical faults, while in this paper we implement the FZTW simulations on vertical or inclined faults and compare their wave fields in both time and frequency domains. The results show that the existence of fault zone and inclined angle of fault can significantly influence the features of waves near faults. In amplitude, a fault zone can generate a larger amplitude of waves. The velocity contrast between two wails of fault may lead to amplification of amplitudes in the low velocity fault wall. In frequency, a fault zone tends to influence the waves in the low frequency range. In a pattern of particle polarization of FZTWs, it tends to be single direction for vertical faults but fork to multiple directions for inclined faults, which might provide a new way to study the fault zone with FZTWs. These conclusions may be valuable for FZ structure inversion, and will enhance the knowledge on near-fault strong ground motions. 展开更多
关键词 Fault zone trapped waves SEM simulation inclined fault Wave fieldcharacteristic
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Dyke Emplacement in the Narmada Rift Zone and Implications for the Evolution of Deccan Traps
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作者 JU Wei HOU Guiting K.R.HARI 《Acta Geologica Sinica(English Edition)》 SCIE CAS CSCD 2016年第S1期157-158,共2页
Dykes are primarily extensional fractures that form perpendicular to the minimum principal compressive stress,which have been extensively studied in the world during the past decades for various reasons including the
关键词 Dyke Emplacement in the Narmada Rift zone and Implications for the Evolution of Deccan traps
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Genetic models of structural traps related to normal faults in the Putaohua Oilfield,Songliao Basin 被引量:3
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作者 Sun Simin Wu Xinsong +1 位作者 Liu Hongtao Wang Changsheng 《Petroleum Science》 SCIE CAS CSCD 2008年第4期302-307,共6页
The Putaohua Oilfield is a fault-prolific area and the faults have close relation with structural traps. The genetic models of the structural traps in the Putaohua Oilfield can be divided into two types: individual f... The Putaohua Oilfield is a fault-prolific area and the faults have close relation with structural traps. The genetic models of the structural traps in the Putaohua Oilfield can be divided into two types: individual fault model and multi-fault interaction model. This is based on the description of displacement distribution of typical individual normal faults, the geometry of the footwall and hanging wall, and the analysis of the interaction between faults and the corresponding change in geometry when the faults grow. The individual fault model is that the displacement reaches a maximum at or near the center of fault and decreases toward the fault tips, so a half-graben is formed on the hanging wall of the fault and a half- anticline is formed on the footwall because of the isostatic process. The multi-fault interaction model is that during the growth of faults, they overlap and interact with each other, and accommodation zones are formed in the overlapping segments. The accommodation zones are favorable targets for hydrocarbon exploration, and the trap characteristics are dependent The multi-fault interaction model can be subdivided on the extent of overlap and occurrence of faults. into three types: synthetic accommodation zone, convergent accommodation zone and divergent accommodation zone. Hydrocarbon migration and accumulation models of each type have been developed. The hydrocarbon migration and accumulation models of the traps with different genetic models have their own characteristics in the different stages of fault growth. 展开更多
关键词 Songliao Basin Putaohua Oilfield accommodation zone normal fault growth structural trap
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增压型走滑转换带对大型圈闭的控制作用——以蓬莱19-3油田为例 被引量:1
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作者 杨波 吴庆勋 +2 位作者 黄振 陈少伟 陈欣怡 《海洋地质前沿》 北大核心 2025年第2期30-42,共13页
蓬莱19-3特大型整装油田是渤海油田郯庐断裂带油气成藏的典型代表之一。目前油田发现三级石油地质储量达10亿t,但对其大型圈闭的形成机制尚无针对性报道。为了弄清蓬莱19-3油田圈闭的成因机制,本研究基于三维地震、钻井、构造正演模拟... 蓬莱19-3特大型整装油田是渤海油田郯庐断裂带油气成藏的典型代表之一。目前油田发现三级石油地质储量达10亿t,但对其大型圈闭的形成机制尚无针对性报道。为了弄清蓬莱19-3油田圈闭的成因机制,本研究基于三维地震、钻井、构造正演模拟、沙箱物理模拟等地质资料分析,认为增压型走滑转换带控制了蓬莱19-3油田大型圈闭的形成,继而进一步探讨了增压型走滑转换带对蓬莱19-3油田大型圈闭的控制机制。蓬莱19-3构造是由多级、多类型转换带共同控制的大型背形构造,具有“间歇式增压隆升”和“排烃期定型”两大特点;其形成的大型圈闭与盖层、烃源岩晚期排烃形成了良好的时空配置关系。转换带研究对今后在走滑断裂带内寻找大中型油气田具有一定的借鉴意义。 展开更多
关键词 蓬莱19-3油田 走滑断裂 增压型走滑转换带 控圈作用
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西湖凹陷西部斜坡带油气成藏主控因素与勘探新领域 被引量:3
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作者 刘志峰 李林致 +2 位作者 李峰 廖计华 祁鹏 《海相油气地质》 北大核心 2025年第1期71-81,共11页
西湖凹陷西部斜坡带油气藏整体呈现“小、断、贫、散”的特征,综合利用录井、测井、地震、生产等多种资料,分析总结西部斜坡带已发现油气的分布规律,提出西部斜坡带具有“南北分区、上下分层、近源富集”的油气分布特点。通过西部斜坡... 西湖凹陷西部斜坡带油气藏整体呈现“小、断、贫、散”的特征,综合利用录井、测井、地震、生产等多种资料,分析总结西部斜坡带已发现油气的分布规律,提出西部斜坡带具有“南北分区、上下分层、近源富集”的油气分布特点。通过西部斜坡带典型油气藏解剖和失利井地质原因分析,认为圈闭和运移是油气成藏的主控因素。构造样式决定圈闭的类型和有效性,进而控制了不同区域的油气藏类型和差异富集;不同油气运移模式和两期充注、蒸发分馏作用控制了研究区近源成藏和“上油下气”的特征。通过成藏条件分析,指出平湖斜坡潜山、天台斜坡北段和杭州斜坡迎翠轩断裂带具有较好的圈闭和运移条件,是西湖凹陷西部斜坡带的勘探新领域。 展开更多
关键词 油气成藏 圈闭类型 主控因素 勘探领域 西部斜坡带 西湖凹陷
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辽河滩海地区西部凹陷成藏条件与成藏模式 被引量:14
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作者 方世虎 徐怀民 +3 位作者 郭召杰 焦翠华 孟卫工 李建明 《石油实验地质》 CAS CSCD 2004年第3期223-228,共6页
岩心分析和测井标定综合分析表明,辽河滩海西部凹陷发育沙三段和沙一二段两套有效烃源岩,主要分布在海南洼陷带。油气输导层主要由断裂(带)、连通的砂砾岩体和不整合面构成,它们或单独、或组合,控制着主要油气富集带的油气输导及聚集成... 岩心分析和测井标定综合分析表明,辽河滩海西部凹陷发育沙三段和沙一二段两套有效烃源岩,主要分布在海南洼陷带。油气输导层主要由断裂(带)、连通的砂砾岩体和不整合面构成,它们或单独、或组合,控制着主要油气富集带的油气输导及聚集成藏。复合圈闭带控制着复合油气聚集带的形成,各复合油气聚集带的成藏条件相互匹配,形成特征油气成藏模式和油气分布规律。 展开更多
关键词 烃源岩 输导层 成藏模式 复合圈闭带 辽河滩海
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破界创生:从“优秀陷阱”到“卓越聚变”
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作者 郑泉水 《中国科学院院刊》 北大核心 2025年第12期2231-2239,共9页
“李约瑟难题”与“钱学森之问”,共同揭示了一个深层结构性矛盾——“优秀陷阱”:传统教育范式长于规模化培养迎合现有标准的优秀人才,却在系统性抑制能够开辟“新大陆”的卓越天才的涌现。面对“2035年建成教育强国、科技强国、人才... “李约瑟难题”与“钱学森之问”,共同揭示了一个深层结构性矛盾——“优秀陷阱”:传统教育范式长于规模化培养迎合现有标准的优秀人才,却在系统性抑制能够开辟“新大陆”的卓越天才的涌现。面对“2035年建成教育强国、科技强国、人才强国”的战略目标与人工智能(AI)技术带来的时代剧变,推动教育范式变革与评价体系重构,已成为一项迫在眉睫的国家战略议题。基于清华大学钱学森班与深圳零一学院16年的实践探索,我们创立了以“内生动力”为主引擎的“创生教育”新范式。文章旨在论证,为破解优秀陷阱必须进一步实现两大核心突破:(1)认知的突破,必须厘清优秀与卓越的本质分野——前者的动力(A型)高度外生,表现为对外部指标与激励的精准响应;后者的动力(X型)则强烈内生,源于内在的好奇心与创造激情,甚至崇高的使命感。(2)机制的突破,必须实施“相态分离”发展战略:在保障主流教育体系稳定高效的同时,于其外开辟受特殊政策与评价体系保护的、随时间进化的“X型人才发展‘特区’”,并构建两套体系间的动态平衡和闭环机制。实践中,深圳零一学院正借助AI技术,探索创建一种跨越时空的“特区”——“量子态生态”组织形态。该形态旨在以极低的边际成本,高效促成X型学生、重大挑战性问题与顶尖导师之间的“核聚变”式反应,从而实现突破性创新人才的群体性可持续涌现。这套经过实践验证的“创生教育”体系,旨在为国家构建一条自主培养卓越创新人才的全新路径,为破解“钱学森之问”提供一套可撬动全局的战略范式与系统解决方案。 展开更多
关键词 优秀陷阱 创生教育 X型/A型二象性 创新人才发展特区
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松辽盆地伸展和反转构造样式 被引量:33
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作者 张功成 朱德丰 周章保 《石油勘探与开发》 EI CAS CSCD 北大核心 1996年第2期16-20,共5页
松辽盆地晚中生代经历了裂谷期、后裂谷期和反转期演化阶段。裂谷期盆地在单剪伸展作用下形成,主要断裂大多向东倾,基本结构单元为半地堑和半地垒,下地壳存在向东缓倾的拆离带。后裂谷期热沉降起主导作用,伴以弱伸展,形成同沉积型... 松辽盆地晚中生代经历了裂谷期、后裂谷期和反转期演化阶段。裂谷期盆地在单剪伸展作用下形成,主要断裂大多向东倾,基本结构单元为半地堑和半地垒,下地壳存在向东缓倾的拆离带。后裂谷期热沉降起主导作用,伴以弱伸展,形成同沉积型正断裂。反转期在北西向压扭力作用下,前期正断裂反倾向运动,形成正反转构造带。裂谷期的深断陷和反转期的背斜带是油气生成、聚集的有利部位。 展开更多
关键词 低角度断层 正断层 同生构造 背斜圈闭 松辽盆地
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汤西断裂的断层围陷波初步研究 被引量:12
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作者 李松林 赖晓玲 +1 位作者 何加勇 田建华 《地震地质》 EI CSCD 北大核心 2007年第2期354-362,共9页
作为断层围陷波方法在城市活断层探测中的首次尝试,我们针对太行山山前断裂带南段的汤西断裂开展了爆炸震源的观测试验。运用数字滤波和频谱分析等技术,由地震记录图分离出了断层围陷波。根据2横测线的观测结果,可确定断层的位置,并可... 作为断层围陷波方法在城市活断层探测中的首次尝试,我们针对太行山山前断裂带南段的汤西断裂开展了爆炸震源的观测试验。运用数字滤波和频谱分析等技术,由地震记录图分离出了断层围陷波。根据2横测线的观测结果,可确定断层的位置,并可推测断层在该处宽度为200~300m。破裂面较宽,可能与其张性特征有关。分频道地震图显示,断层围陷波具有正频散现象,其低频分量传播较快。这表明断层围陷波是一种面波,可利用其频散规律研究断裂带内介质的物理性质。这次的观测结果也表明,断层围陷波并不局限于新破裂带,在老断层中也能形成和传播。事实上,只要断层带内外的介质在物理性质上有较大的差异,均能产生沿断层传播的围陷波。在城市活断层探测中,断层围陷波的方法具有非常独特的优越性。 展开更多
关键词 断层围陷波 活断层 断层破碎带 汤西断裂
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海原断裂带断层通道波观测与破碎带宽度 被引量:15
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作者 刘明军 李松林 +2 位作者 张先康 樊计昌 宋占龙 《物探与化探》 CAS CSCD 2004年第6期549-552,共4页
断层通道波是低速断层破碎带与高速围岩之间的边界相干多重反射形成的,其振幅和频率强烈依赖于断层的几何形态和物理性质,故能用于探测断裂带的内部结构。在宁夏海原西安州附近海原断裂带上,横跨1920年海原8.6级地震地表破裂带布设2条测... 断层通道波是低速断层破碎带与高速围岩之间的边界相干多重反射形成的,其振幅和频率强烈依赖于断层的几何形态和物理性质,故能用于探测断裂带的内部结构。在宁夏海原西安州附近海原断裂带上,横跨1920年海原8.6级地震地表破裂带布设2条测线,接收测线之间人工爆破激发的断层通道波。每条测线由14台3分量数字地震仪组成,靠近破裂带台间距30~40m,远离破裂带台间距增大至230~250m。对测线1的台站接收到的一炮垂直道地震波数据进行了0.1~4.0Hz频段的滤波,结果表明在S波到时之后存在多组强振幅、低频率、长波链的断层通道波。由断层通道波揭示的海原断裂带在西安州附近的断裂破碎带宽度约为250m。 展开更多
关键词 海原断裂带 断层通道波 破碎带宽度 细结构
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昆仑山断层围陷波的分析和研究 被引量:18
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作者 楼海 王椿镛 +3 位作者 丁志峰 何正勤 杨建思 周民都 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2006年第3期788-796,共9页
对2001年昆仑山口西Ms8.1级地震产生的断层带,布设了沿断层和横跨断层的两条人工地震测线.通过对观测资料的定量分析和处理,求得了昆仑山断层带内部的细结构.分析工作包括从S波震相开始的振幅谱计算、速度频散计算、群速度测量,并用面... 对2001年昆仑山口西Ms8.1级地震产生的断层带,布设了沿断层和横跨断层的两条人工地震测线.通过对观测资料的定量分析和处理,求得了昆仑山断层带内部的细结构.分析工作包括从S波震相开始的振幅谱计算、速度频散计算、群速度测量,并用面波频散方法反演S波速度结构,用振幅谱比的方法估计断层带的Q值.野外试验结果表明,S波震相与围陷波组的时间差随炮点与台站之间距离增大而增加,在断层带外的测点上观测到与断层带相关的场地效应.最后得出昆仑山断层带宽度为250m、速度结构为断层内低速的分层结构和Q值为15(断层内)和30(围岩).虽然昆仑山口西地震的震级比美国加州Landers地震的震级(Ms7.6)大,且地震产生的破裂带长度长得多,但是这两个地震断层带的宽度却相差不大. 展开更多
关键词 断层带 围陷波 人工爆破 速度结构 面波频散
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确定断裂带内部结构和物性参数的一种方法 被引量:13
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作者 樊计昌 刘明军 《石油地球物理勘探》 EI CSCD 北大核心 2007年第2期164-169,共6页
上地壳的深大断裂在地下深处常常伴有几百米至几千米宽的低速带,它对油气的储集和运移或对储层的破环起着重要的控制作用。了解其三维形态、规模、倾向及物性参数(如波速和Q值等),对指导油气勘探有重要作用。断层带围陷波方法是精确确... 上地壳的深大断裂在地下深处常常伴有几百米至几千米宽的低速带,它对油气的储集和运移或对储层的破环起着重要的控制作用。了解其三维形态、规模、倾向及物性参数(如波速和Q值等),对指导油气勘探有重要作用。断层带围陷波方法是精确确定断层几何形态和物性参数的一种有效方法。本文给出了确定断裂带内部物性参数的计算公式和步骤,开发了一套综合利用断层带围陷波和体波(P波和S波)确定断层几何形态和物性参数的软件,还给出了围陷波分析和计算的应用实例。研究及应用结果表明:通过谱分析方法,利用断层带围陷波能够初步确定断层的结构、随深度的延续特征及物性参数;借助于围陷波和体波的走时及波形资料,利用谱分析和射线追踪方法可进一步确定断层的三维几何形态和物性参数。 展开更多
关键词 断层带围陷波 断裂带内部结构 谱分析 物性参数 射线追踪 人机交互软件
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准噶尔盆地石南地区J_1s_2~1砂组沉积相带展布及岩性圈闭识别 被引量:3
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作者 任小军 于兴河 +2 位作者 李胜利 岳云雷 李瑞军 《天然气地球科学》 EI CAS CSCD 2008年第6期805-809,共5页
石南地区位于准噶尔盆地腹部,其J1s21砂组为湖侵体系域沉积,砂体发育,储盖层配置良好,是该区岩性圈闭发育的有利层位。以井、震资料为基础并综合多种沉积参数,研究了该区J1s21砂组的精细沉积相,并分析了岩性圈闭的主控因素,预测了岩性... 石南地区位于准噶尔盆地腹部,其J1s21砂组为湖侵体系域沉积,砂体发育,储盖层配置良好,是该区岩性圈闭发育的有利层位。以井、震资料为基础并综合多种沉积参数,研究了该区J1s21砂组的精细沉积相,并分析了岩性圈闭的主控因素,预测了岩性圈闭发育的有利区带,最后,以夏盐3井岩性圈闭作为实例,对其储盖组合、成藏条件进行了评价。 展开更多
关键词 精细沉积相 岩性圈闭 有利发育区带 石南地区
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辽河滩海地区西部凹陷古近系岩性和地层圈闭形成条件与发育模式 被引量:10
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作者 周宗明 于炳松 +2 位作者 张聪 王宏语 张迪 《油气地质与采收率》 CAS CSCD 北大核心 2011年第1期11-14,111-112,共4页
通过三维地震资料解释,结合区域地质背景及层序发育、沉积充填演化特点,对辽河滩海地区西部凹陷古近系岩性和地层圈闭的形成条件及发育模式进行了研究。结果表明,研究区发育砂岩透镜体圈闭和地层超覆圈闭,其中砂岩透镜体圈闭可分为低位... 通过三维地震资料解释,结合区域地质背景及层序发育、沉积充填演化特点,对辽河滩海地区西部凹陷古近系岩性和地层圈闭的形成条件及发育模式进行了研究。结果表明,研究区发育砂岩透镜体圈闭和地层超覆圈闭,其中砂岩透镜体圈闭可分为低位浊积扇圈闭、高位滑塌扇圈闭和近岸水下扇圈闭。沉积坡折和断裂坡折是各体系域中岩性、地层圈闭砂体发育的主要条件,岩性、地层圈闭发育模式以低位体系域及高位体系域发育透镜体圈闭、湖侵体系域发育地层超覆圈闭为主。 展开更多
关键词 岩性圈闭 地层圈闭 坡折带 层序 发育模式 辽河坳陷
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