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南北地震带中段地震活动的板块动力学研究 总被引:2,自引:0,他引:2
在大陆造山带研究的最新成果基础上论述了南北地震带中段地壳的定变过程,结合造山带内部的高温韧性滑脱构造及地球物理深部探测成果和新生代以来的板块运动探讨了南北地震 段地震的地壳动力学过程及成因机制。 相似文献
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天山的晚新生代构造变形及其地球动力学问题 总被引:73,自引:6,他引:73
天山是大陆内部典型的新生代复活造山带,其新生代构造变形的方式,变形量,速度及过程等对于认识大陆内部造山带的变形机理有着重要的意义。本文在对南北天山主要活动构造地质填图和综合研究的基础上,重点探讨了天山的晚新生代构造变形特征及其动力学问题。早更新世以来,特别是早,中更新世之间,天山的构造活动由内部向南北两侧扩展,使得两侧的新生代凹陷逐渐褶皱成山,形成数排新生代褶皱带,整个天山的现代构造活动是一种扇形 相似文献
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中国大陆西北造山带及其毗邻盆地的地震层析成像 总被引:41,自引:6,他引:35
根据新疆、甘肃、青海和吉尔吉斯斯坦地震台网提供的地震数据,利用地震层析成像法重建了中国大陆西北造山带及其毗邻盆地的地壳上地幔三维速度图像.上地壳造山带大都为高速区,盆地和地陷区的低速显然与较厚的松散沉积层有关.地壳中部东、西天山之间存在低速边界,造山带及青藏高原北部的莫霍面深度较大,盆地和坳陷区的莫霍面相对较浅.上地幔软流层在青藏高原、阿尔泰山、祁连山等地较浅,在塔里木盆地和天山一带较深.地幔热物质有可能在板块碰撞中沿构造边界上升到造山带的底部,它们的动力学性质与中国大陆西北造山带的形成演化有着密切的联系。 相似文献
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天山南北前陆盆地新生代变形与天山造山带的波动耦合 总被引:1,自引:0,他引:1
天山南北前陆盆地变形及与天山构造变动的关系一直备受关注.通过地震资料解释和地面地质调查,对它们的构造特点、构造样式、变形主控因素、变形时间和关系等进行了对比研究.两个前陆盆地新生代变形都表现出南北分带、东西分段和上下分层的特点.变形样式以压性为特点,既有基底卷入式变形,也有盖层滑脱式变形.这种变形的复杂性与软性地层的存在有密切关系.从变形时间上看,新生代两个盆地都经历了多期变形,且变形表现为从天山造山带向盆地内部逐渐变新.天山南北前陆盆地的变形动力学可用造山楔动力学模型代表,但其构造又明显表现出波的特点,据此提出了波动造山楔的概念,建立了天山两侧双波动楔模型. 相似文献
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从时空展布和应变积累释放角度,对中国大陆及大陆西部和东部地区地震活动进行分析,认为青藏高原地震区是中国大陆强震活动主体区域,在目前空间格局不发生改变的情况下,巴颜喀拉地块区及边界、川滇地区是强震活动主要场所的可能性较大;其次为新疆地震区,其强震主体区域依次为南天山与西昆仑交汇区、阿尔泰地区、南北天山地区;中国大陆东部目前可能处于第2轮回后剩余释放阶段或可能已进入第3个轮回的应变积累阶段,总体应变积累水平较低,发生强地震的可能性较小,若进入活跃期,华北地震区应是M≥6.0地震活动的主体区域。 相似文献
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利用1992~2012年多期境内外天山西南地区GPS观测数据,计算得出天山西南及帕米尔地区现今构造变形运动速度场,并计算给出了研究区内最大主应变、剪应变率和面膨胀的分布情况。结果表明:在西天山地区受印度板块西构造结挤压作用下,帕米尔高原快速向北俯冲,造成天山沿这一经度带发生了强烈的地壳缩短;盆—山结合带的变形大于山体内部变形,形变幅度最大的地方往往就是历史上多次发生7~8级大震的地方;天山主压应变方向随经度增加逐渐由北北西向转向南北及北北东向,基本上与天山山脉走向垂直;主压应变较大的地区集中在西天山南北褶皱带上,最大剪应变率位于西天山南缘与帕米尔高原及西昆仑结合部,高值区是强地震的主要分布区。 相似文献
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中国大陆西部未来强震危险性预测研究 总被引:8,自引:4,他引:4
主要研究中国大陆西部(E107°以西)区域中长期地震危险性和可能发生强震的区域.文中选用了可靠时段地震目录,应用震级-频度关系,计算6级以上各震级段年优势发生次数,对近100年以来的7级以上地震的地震波能量进行统计和分析,并利用近30年来地震震源机制解计算应力场的方向.结合断裂构造、应力场方向、缺震次数及不同区域的能量释放情况,认为中天山南北区域、中印巴三国交界区域、青甘藏川交界区域及祁连地震带(即南北地震带中段和北段)等几个区域应为未来的重点监测区域. 相似文献
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《Advances in water resources》2005,28(7):701-710
The patterns of temporal variations of precipitation (P), streamflow (SF) and baseflow (BF) as well as their nitrate-nitrogen (nitrate) concentrations (C) and loads (L) from a long-term record (28 years) in the Raccoon River, Iowa, were analyzed using variogram and spectral analyses. The daily P is random but scaling may exist in the daily SF and BF with a possible break point in the scaling at about 18 days and 45 days, respectively. The nitrate concentrations and loads are shown to have a half-year cycle while daily P, SF, and BF have a one-year cycle. Furthermore, there may be a low-frequency cycle of 6–8 years in C. The power spectra of C and L in both SF and BF exhibit fractal 1/f scaling with two characteristic frequencies of half-year and one-year, and are fitted well with the spectrum of the gamma distribution. The nitrate input to SF and BF at the Raccoon watershed seems likely to be a white noise process superimposed on another process with a half-year and one-year cycle. 相似文献
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燕郊等测点迁移优化与地磁观测研究 总被引:1,自引:2,他引:1
为优化地磁观测条件,开展了燕郊、夏垫等测点迁移工作;按照测眯迁移原则与实施技术方案,完整地收集并整理了地质构造与地球物理等方面的基本资料;进行了野外实地勘察,磁场梯度的测量,确定了新测点,在新老测点上进行了较长时间的地磁场对比观测;应用多种方法分析研究了地磁对比观测资料,结果表明,新老测点与有关测点的地磁变化具有良好的一致性,并得到了新老测点之间的地磁数据的按点差。 相似文献
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We rederive and generalize hyperbolic moveout formulae for the common-midpoint (CMP) gather and for the zero-offset (ZO) section that can be efficiently used for macro-model-independent reflection imaging in two-dimensional media. The hyperbolic moveout formulae for the common-midpoint gather are obtained from different Taylor series expansions of a particular parametric moveout surface defined in the multicoverage data space. Such a moveout surface involves three kinematic wave-field attributes of two hypothetical waves, which have to be determined by a coherency analysis. By using hyperbolic moveout curves in the CMP gather and in the ZO section one can determine these attributes in two steps. The relationships between the local shapes of the interfaces and the attributes of the hypothetical wave-fields attributes are considered by means of geometrical optics. The determination of these attributes allows to perform a macro-model-independent ZO simulation and a subsequent inversion. 相似文献
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Vindell Hsu Charles E. Helsley Eduard Berg David A. Novelo-Casanova 《Pure and Applied Geophysics》1984,122(6):878-893
A close correlation in spatial distribution of local seismic activity and energy release patterns before and after the 1979 Petatlan, Mexico earthquake suggests heterogeneity within the fault plane of this major low-angle thrust event associated with subduction along the Middle America Trench. A simple two-asperity model is proposed to account for the complexity. Foreshocks and aftershocks of the neighboring 1981 Playa Azul earthquake showed a similar pattern. As both events occurred at the junction of the Orozco Fracture Zone and the Middle America Trench, we speculate that the observed complex fault plane is caused by subduction of the rugged ocean floor of the Orozco Fracture Zone. Short-term precursory seismicity prior to the Petatlan earthquake can be explained by using the asperity model and migration of a slip front from the south-east to the north-west across the main shock source region. 相似文献
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Summary This paper discusses the influence of system stiffness on the dynamic instability of fault surfaces under laboratory conditions for a number of test modes. In conjunction with shear load stiffness, the normal load stiffness, often neglected, is shown to have a considerable effect on the stick-slip process —its presence or absence and its characteristics. Also appropriate stiffnesses are suggested for an earthquake sequence modeled as a growing dislocation. 相似文献