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时间项分析法中，应用广义最小二乘法进行反演，对长白山天池火山区岩浆系统的长白—敦化(L1)剖面的Pg波到时进行了计算处理，得到了Pg波时间项及基底速度值；取上部地壳的介质平均速度为4．5km/s，经反演求得了各点的深度值，给出了长白山天池火山区结晶基底的厚度分布。结晶基底厚度一般在2．0km左右，而在长白山天池下方结晶基底最厚处接近4．0km；在万宝和敦化附近各有一不太明显的凹陷，其原因可能与在这两个位置处有几条断裂穿过有关。 相似文献
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对三峡地区的Ｐｇ波非纵观测资料用地震层析成象方法进行了计算处理并对解释结果作了分析。简要阐述了地震析成象处理方法，地震走时数据的采集与分析等。基底面成象图给出了许多有意义的信息；该测区低速区的开矿要起因于岩性的差异及断层破碎带；基底面上存在３个ｖ〉６．４ｋｍ／ｓ的高速度区，面积最大的一个大体呈南北走向，位于黄陵背斜西南侧、向北进入背斜区，另两个分别位于黄陵背斜东则与测区西侧。 相似文献
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利用六面体单元和三线性插值函数，推导出在任意弹性各向异性介质中三维三分量波动方程所满足的有限元方程．给出用时域有限差分求解该有限元方程时，时间、空间采样率和弹性参数应满足的稳定性条件．提出避免每一时间步都求解一大型线性代数方程组的方法．在开始求波场前，先求质量矩阵的逆的因子形式，以后每时间步只需作刚度矩阵的逆的因子形式与向量的乘积运算，可大大提高有限元素法在微机上进行波动方程数值模拟的运算速度．结合两个数值模拟算例，说明该方法的可行性，并与伪谱法作了计算速度的比较，有限元法的计算速度高于伪谱法的计算速度． 相似文献
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井间电阻率层析成象的某些进展 总被引：7，自引：2，他引：7
用有限元法作电阻率层析成象的核心问题是Ｊａｃｏｂｉ矩阵的求取和反演成象算法的研究。本文主要论述了这两方面的最新进展，即求取Ｊａｃｏｂｉ矩阵的格林函数法，用于反演成象计算的平滑度约束反演。文中通过理论模型的成象计算，比较了两种反演算法的成象效果。 相似文献
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华北地区上部地壳结构的三维有限差分层析成像 总被引：34，自引：12，他引：22
采用正方形网格对华北地区速度模型进行参数化、网格维数为649×90×16,网格间距为1km. 通过对华北地区30条深地震测深剖面的Pg波三维有限差分速度层析成像反演,获得了该地区上部地壳的三维速度结构. 反演结果显示,低速的"棱形"华北盆地被高速的隆起所包围;而华北盆地又由两个大的断陷带中间夹一个隆起所组成.两个大的断陷带又被分割为多个小的断陷盆地.研究区内的断层多为铲式正断层,结晶基底深度变化较大. 所有这些表明华北地区具有复杂的地质构造和发生强震的深部背景. 相似文献
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在深度偏移方法中，把二维隐式方法推广到三维，就会面对一个分块对角矩阵求逆问题. 通常，这种矩阵的求逆将耗费大量计算时间，严重制约了三维隐式方法偏移在实际资料处理中的广泛应用. 在螺旋边界条件下，该矩阵H具有Toeplitz结构的正定厄密矩阵，其快速求逆可由谱法LU分解或直解法快速实现. 本文结合谱法LU分解和直接解法方法的优点，提出了一种混合算法. 文中采用谱分解方法建立起矩阵列元素的谱分解表，并采用直解法的递推公式，可以快速给出矩阵的分解. 通过与谱法分解和直解法在分解精度和分解速度两方面的比较表明，本文方法与谱法相比，在非均匀介质中亥姆霍兹算子矩阵分解时的精度提高10倍；在计算速度方面，混合方法比简化后的直解法快. 因此，该方法的提出，在计算精度许可的条件下，最大限度地减少三维隐式差分偏移中矩阵求逆占用的时间，从而使得该方法能真正用于实际地震资料的处理. 相似文献
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基于稳定电流场的基本方程、三维区域满足的边值问题以及相应的变分问题，研究了三维起伏地形条件下电阻率的有限单元数值模拟算法. 离散积分区域时，以三棱柱为最小研究单元，推导了含有地形特征信息的三线性插值型函数以及单元刚度矩阵. 采用变带宽、一维数组方式只存储稀疏刚度矩阵中非零元素，能够节约内存. 利用Cholesky分解法只分解一次大型稀疏矩阵，通过回代可以求出方程组的全部解，当求解有多个供电点的测深问题时可以缩短计算时间. 模型计算表明，在水平层状介质模型上，三维计算结果与解析解或二维数值解十分吻合，计算精度满足误差要求. 在二维山脊上的二极剖面或三维山谷上的中间梯度剖面上，其三维计算结果与相应模型的土槽实验结果或边界元法计算结果也非常接近. 相似文献
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本文讨论了弹性波瞬态传播问题的三维有限元计算方法及当前存在的实际困难.针对要求计算机内存大和计算时间长的问题,采取了改进措施.由于采用了集中质量矩阵和修正的中心差分时间积分显格式相结合的方法,可以使计算机内存和计算时间大为减少;由于采用结点定位法,最适合用于目前发展的并行计算机系统,可使计算速度大大增快;还采用了有效激发震源法,有效激发区是随时间步进的增加而逐步增大,这不仅能节省计算时间,而且使波场的传播过程一目了然,本文计算了由两种介质组成的三维楔形问题,得到若干典型剖面的瞬时波场图及随时间变化的合成地震图. 相似文献
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Waruntorn Kanitpanyacharoen Hans‐Rudolf Wenk Frans Kets Christian Lehr Richard Wirth 《Geophysical Prospecting》2011,59(3):536-556
Scanning and transmission electron microscopy, synchrotron X‐ray diffraction, microtomography and ultrasonic velocity measurements were used to characterize microstructures and anisotropy of three deeply buried Qusaiba shales from the Rub’al‐Khali basin, Saudi Arabia. Kaolinite, illite‐smectite, illite‐mica and chlorite show strong preferred orientation with (001) pole figure maxima perpendicular to the bedding plane ranging from 2.4–6.8 multiples of a random distribution (m.r.d.). Quartz, feldspars and pyrite crystals have a random orientation distribution. Elastic properties of the polyphase aggregate are calculated by averaging the single crystal elastic properties over the orientation distribution, assuming a nonporous material. The average calculated bulk P‐wave velocities are 6.2 km/s (maximum) and 5.5 km/s (minimum), resulting in a P‐wave anisotropy of 12%. The calculated velocities are compared with those determined from ultrasonic velocity measurements on a similar sample. In the ultrasonic experiment, which measures the effects of the shale matrix as well as the effects of porosity, velocities are smaller (P‐wave maximum 5.3 km/s and minimum 4.1 km/s). The difference between calculated and measured velocities is attributed to the effects of anisotropic pore structure and to microfractures present in the sample, which have not been taken into account in the matrix averaging. 相似文献
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沿乌鲁木齐－库尔勒３５０余公里长的测线上完成了穿越天山的地震转换波野外观测，得出天山造山带的深部构造剖面图和壳内Ｐ，Ｓ波速度结构模型．天山的结晶地壳可分为４层，各层的速度分别是：Ｖｐ值为５．９，６．３，６．６，６．９ｋｍ／ｓ；Ｖｓ值为３．２，３．５，３．７，３．９ｋｍ／ｓ。上地幔顶部的波速：Ｖｐ值为８．１０ｋｍ／ｓ。Ｖｓ值为４．６ｋｍ／ｓ。天山地区的地壳厚度为４２－５６ｋｍ，中天山最厚，达到５０－５６ｋｍ。地壳中部存在低速透镜体。探测结果表明，天山大地构造可分为北天山、中天山和南天山３个区，其地壳深部构造特征各不相同。用颤动构造理论来解释天山造山带的形成机制和演化较板块构造理论更为合理。 相似文献
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沿乌鲁木齐－库尔勒３５０余公里长的测线上完成了穿越天山的地震转换波野外观测，得出天山造山带的深部构造剖面图和壳内Ｐ，Ｓ波速度结构模型．天山的结晶地壳可分为４层，各层的速度分别是：Ｖｐ值为５．９，６．３，６．６，６．９ｋｍ／ｓ；Ｖｓ值为３．２，３．５，３．７，３．９ｋｍ／ｓ。上地幔顶部的波速：Ｖｐ值为８．１０ｋｍ／ｓ。Ｖｓ值为４．６ｋｍ／ｓ。天山地区的地壳厚度为４２－５６ｋｍ，中天山最厚，达到５０－５６ｋｍ。地壳中部存在低速透镜体。探测结果表明，天山大地构造可分为北天山、中天山和南天山３个区，其地壳深部构造特征各不相同。用颤动构造理论来解释天山造山带的形成机制和演化较板块构造理论更为合理。 相似文献
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Field measurements of seismic P-wave velocities have been carried out by surface to surface refraction measurements for five different rock types. Subweathering velocities are surprisingly high and range from 5.0 km/sec in quartz monzonite to 6.2 km/sec in amphibolite in agreement with the proposal of Nur and Simmons for water-saturated low-porosity rocks. Maximum velocities found are 6.1 km/sec for quartz monzonite, 5.8 km/sec for granite gneiss, 6.4 km/sec for syenite, 6.4 km/sec for anorthosite, and 7.0 km/sec for amphibolite, and maximum depth for these velocities is 1.3 km. We conclude as follows: (1) field measurements correspond well with laboratory measurements but true velocity may be slightly higher than laboratory measurements, (2) shallow velocities are much higher than older laboratory measurements but agree well with recent laboratory measurements on water-saturated samples, (3) velocities much less than 6 km/sec seem unlikely in the crust unless in an area of extreme tectonic activity, (4) velocities of 6.5–6.7 km/sec commonly reported for the lower continental crust probably correspond to rocks less mafic than basalt or gabbro. 相似文献
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A direct measurement of apparent velocities for oceanic paths was made with an array of sensitive ocean bottom seismographs. The measurement was performed by recording waves from shallow earthquakes which occurred in the area close to trench axes and which were accurately located by the land seismological network in Japan. The range of epicentral distances is from 500 to 1,800 km.The observed P travel times are less than those in the Jeffreys-Bullen tables by 6–10 s for the range of distances.Since the dimension of the OBS array is about 400 km, the apparent velocities are determined quite precisely and show little dependence on the epicentral distances. The average value of the apparent velocities for the range 500–1,700 km is 8.64 ± 0.13 km/s.An offset of travel times, which is thought to be associated with a low-velocity layer underneath the oceanic lithosphere, has been observed.These results indicate that a high-velocity layer with a velocity of 8.6 km/s exists in the lower part of the oceanic lithosphere. Beneath the 8.6-km/s layer there is a thin low-velocity layer under which the velocity of the P wave is again 8.6 km/s. 相似文献
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Surface wave dispersion is studied to obtain the 1-D average velocity structure of the crust in the Korean Peninsula by inverting
group- and phase-velocities jointly. Group velocities of short-period Rayleigh and Love waves are obtained from cross-correlations
of seismic noise. Multiple-filter analysis is used to extract the group velocities at periods between 0.5 and 20 s. Phase
velocities of Rayleigh waves in 10- and 50-s periods are obtained by applying the two-station method to teleseismic data.
Dispersion curves of all group and phase velocities are jointly inverted for the 1-D average model of the Korean Peninsula.
The resultant model from surface wave analysis can be used as an initial model for numerical modeling of observations of North
Korean events for a velocity model appropriated to the Korean Peninsula. The iterative process is focused especially on the
surface sedimentary layer in the numerical modeling. The final model, modified by numerical modeling from the initial model,
indicates that the crust shear wave velocity increases with depth from 2.16 km/s for a 2-km-thick surface sedimentary layer
to 3.79 km/s at a Moho depth of 33 km, and the upper mantle has a velocity of 4.70 km/s. 相似文献
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The phase velocities of Rayleigh waves and the lateral variation of lithospheric structure in Tibetan Plateau 总被引：1，自引：0，他引：1
According to a Sino-U. S. joint project, eleven broadband digital PASSCAL seismometers had been deployed inside the Tibetan
Plateau, of which 7 stations were on the profile from Lhasa to Golmud and other 4 stations situated at Maxin, Yushu, Xigatze
and Linzhi. Dispersions and phase velocities of the Rayleigh surface waves (10s–120s) were obtained on five paths distributed
in the different blocks of Tibetan Plateau. Inversions of the S-wave velocity structures in Songpan-Ganzi block, Qiang-Tang
block, Lhasa block and the faulted rift zone were obtained from the dispersion data. The results show that significant lateral
variation of the S-wave velocity structures among the different blocks exists. The path from Wenquan to Xigatze (abbreviated
as Wndo-Xiga) passes through the rift-zone of Yadong-Anduo. The phase velocities of Rayleigh waves from 10s to 100s on this
path are significantly higher than that on other paths. The calculated mean crustal velocity on this path is 3.8 km/s, much
greater than that on other paths, where mean crustal velocities of 3.4–3.5 km/s are usually observed. Low velocity zones with
different thicknesses and velocities are observed in the middle-lower crust for different paths. Songpan-Ganzi block, located
in the northern part of Tibetan Plateau is characterized by a thinner crust of 65 km thick and a prominent low velocity zone
in the upper mantle. The low velocity zone with a velocity of 4.2 km/s is located at a depth form 115 km to 175 km. While
in other blocks, no low velocity zone in the upper mantle is observed. The value of Sn in Songpan-Ganzi is calculated to be
4.5 km/s, while those in Qiang-Tang and Lhasa blocks are about 4.6 km/s.
The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, Supp., 566–573, 1992. 相似文献
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根据阿尔泰—阿尔金地学断面的地震纵、横波资料,建立了地壳速度及泊松比结构. 测区的地壳具有明显的三分结构特征,其纵波速度自上而下依次为6.0～6.3km/s、6.3～6.6km/s及6.9～7.0km/s;阿尔泰南缘的地壳最厚,为56km,准噶尔盆地的地壳最薄,为46km,大部分地区的地壳厚度为50km 左右. 准噶尔盆地与天山之间上地幔顶部的纵波速度为7.7～7.8km/s ;阿尔泰南缘及塔里木盆地上地幔顶部的纵波速度较高,为7.9～8.0km/s. 测线南部,包括东天山及塔里木东缘,自地表至30km深处的地壳纵波速度低,泊松比为0.25,表明上地壳主要为石英及花岗质成分;而测线北部(包括阿尔泰及准噶尔盆地)的中、上地壳则呈现较高的泊松比（0.26～0.27）,可能为基性地壳的体现. 厚15～30km的下地壳纵波速度（6.9～7.0km/s）较高,泊松比为0.26～0.28,可能以镁铁质的麻粒岩成分为主. 位于天山及其南侧地壳中部的低速层（VP=5.9km/s, σ=0.25）则可能为晚古生代的构造热事件中的花岗质侵入岩. 相似文献
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Velocity structure of the upper mantle of the East European platform according to seismic noise data
T. Yu. Koroleva T. B. Yanovskaya S. S. Patrusheva 《Izvestiya Physics of the Solid Earth》2010,46(10):839-848
Cross-correlation functions of noise are constructed on 119 interstation paths from seismic noise records at stations of Eastern Europe. Dispersion curves of the group velocity of Rayleigh waves obtained from the cross-correlation functions are used for constructing the three-dimensional distribution of the velocity of transverse waves on the East European platform and in adjacent regions by methods of surface-wave tomography. The mean velocity in the crust is minimum in the region of the Caspian depression and Black Sea basin (<3.3 km/s) and maximum in the Baltic shield area (>3.7 km/s). The upper mantle beneath the Baltic and Ukrainian shields is characterized by increased velocity and the absence of the asthenospheric layer. Reduced velocities are noted in the upper mantle of the Black Sea basin. A low-velocity anomaly in the shape of a vertical column is revealed at depths of 200–300 km in the central part of the Dnieper-Donets aulacogen, which confirms the existence of a paleorift in this region. 相似文献