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1.
本文试图采用卫星重力资料和一种新的反演方法来研究地幔的横向密度异常分布.先将密度异常△(r,,(?))在一个三维正交函数系下进行展开,其展开系数待定.然后,根据密度异常与重力扰动位之间的关系建立观测方程组,其中未知向量由密度异常展开系数组成,重力扰动观测向量由 GEM10B 重力模型中的位系数计算而得,并通过适当选取重力位系数的阶数,对观测向量进行滤波.最后,就下地幔(670km——CM 界面)作了实际计算.计算中,重力扰动位阶数取为2——11阶,密度异常展开式的截断阶数取为 K=4和 L=6,求解观测方程组时采用阻尼最小二乘法.结果表明:密度扰动值在670km 不连续面及核幔界面处达到极大值,且在环太平洋地区存在一高密度带,太平洋中部对应于一低密度区,这些特征与 Dziewonski 得到的下地幔三维波速异常分布特征相一致.但是,在南极地区、大西洋及印度洋部分地区,所得的密度异常分布与三维波速异常分布呈负相关,文章就其原因作了初步分析.   相似文献   

2.
重力位球谐系数及板块运动速度是两种独立的地球物理观测资料,但二者同时又是地幔内横向密度差异及与之相联系的地幔流动的结果,从而,中长波重力异常与板块运动的观测提供了探索地幔横向非均匀的一条途径。本文根据适合于低雷诺流动的最小粘滞损耗原理,利用张量场及矢量场的标量分解与传播子解的数学方法,将观测的重力位球谐系数和板块运动速度作为约束条件,发展了一种反演地幔横向密度差异的方法。  相似文献   

3.
Introduction The gravity anomaly is an indicator of the density distribution of the underground material. Therefore the gravity anomalies have been important data used for studying the deep crustal struc-ture for a long time. Many people have made detailed researches on the regional crustal structure inverted by Bouguer anomalies. In particular some empirical formulae and practical algorithms about the crustal thickness were brought forward, and a series of results were obtained (MENG, 1996)…  相似文献   

4.
To reduce the numerical complexity of inverse solutions to large systems of discretised integral equations in gravimetric geoid/quasigeoid modelling, the surface domain of Green’s integrals is subdivided into the near-zone and far-zone integration sub-domains. The inversion is performed for the near zone using regional detailed gravity data. The farzone contributions to the gravity field quantities are estimated from an available global geopotential model using techniques for a spherical harmonic analysis of the gravity field. For computing the far-zone contributions by means of Green’s integrals, truncation coefficients are applied. Different forms of truncation coefficients have been derived depending on a type of integrals in solving various geodetic boundary-value problems. In this study, we utilise Molodensky’s truncation coefficients to Green’s integrals for computing the far-zone contributions to the disturbing potential, the gravity disturbance, and the gravity anomaly. We also demonstrate that Molodensky’s truncation coefficients can be uniformly applied to all types of Green’s integrals used in solving the boundaryvalue problems. The numerical example of the far-zone contributions to the gravity field quantities is given over the area of study which comprises the Canadian Rocky Mountains. The coefficients of a global geopotential model and a detailed digital terrain model are used as input data.  相似文献   

5.
由Hager(1981)提出的,叶正仁(1989)进一步发展的传播矩阵方法,提供了一种运用地球重力位、板块运动速度资料来探求地幔内部横向不均匀性的一条途径.但由于地球重力位、板块运动速度资料均是二维资料,故仅运用上述两种资料来反演三维异常密度会导致反演结果很强的不唯一性、不稳定性.作为80年代地球物理学最富有成效的成果之一就是利用地震P 波和S波的层析技术,提供了上、下地幔三维异常速度分布,从而为地球物理及地球动力学的研究提供了最新的先验知识.把传播矩阵方法、粘滞损耗最小原理运用于全地幔对流的地球动力学模型,并同时把长波地形起伏、板块运动速度、重力位资料以及傅容珊根据地震层析结果所合成的全地幔三维异常密度作为约束条件,联合反演全地幔的三维异常密度结构.计算结果显示:(1)从计算所及的密度横切剖面来看,至少在250—670km 深度范围内异常密度的高低与地表构造有一定的相关性:即全球的大部分发散边界和相当部分的大陆分别对应低异常密度区和高异常密度区,地幔的异常密度数值在1500km 深度附近达到最小.(2)从计算所得的密度纵切剖面来看,对应太平洋中脊、印度洋中脊、红海及亚丁湾地区,低密度的异常区从地表一直延伸到核一幔边界,不过太平洋中脊相对明显.除上述区域外全地幔的异常密度基本上(按数值大小及正负)分三层.  相似文献   

6.
This paper presents systematic studies on the C—O and Sr—Nd isotopic compositions for Cretaceous Badou carbonatites, Fangcheng basalts, and Jiaodong lamprophyres and Paleozoic Mengyin kimberlites in Shandong Province, China. Paleozoic kimberlites have normal and uniform C—O isotopic compositions with δ13C and δ18O in the range of −4.8‰—−7.6‰ and +9.9‰—+13.2‰, respectively. However, Cretaceous three different types of mantlederived rocks have quite different C—O isotopic compositions, indicating that the mantle sources are probably partially contaminated with organic carbon-bearing crustal materials. These Cretaceous rocks show uniform and EMII-like Sr—Nd isotopic compositions and also indicate that the mantle sources were affected by recycled crustal materials. Comparative studies of C—O and Sr—Nd isotopes reveal that the lithospheric mantle beneath the eastern North China Craton had different isotope characteristics in the Paleozoic, the early Cretaceous, and the Tertiary time. This demonstrates that the lithospheric mantle beneath the region underwent at least twice reconstructions since the Paleozoic. Available data imply that the first reconstruction mainly happened during the Triassic-Jurassic time with gradual changes and the second in the Cretaceous with abrupt changes. Results also show that the early Cretaceous (especially at 120-130 Ma) was perhaps the key period leading to the dramatic change of the Mesozoic geodynamics on the eastern North China Craton.  相似文献   

7.
In this study, the KLME approach, a moment-equation approach based on the Karhunen–Loeve decomposition developed by Zhang and Lu (Comput Phys 194(2):773–794, 2004), is applied to unconfined flow with multiple random inputs. The log-transformed hydraulic conductivity F, the recharge R, the Dirichlet boundary condition H, and the Neumann boundary condition Q are assumed to be Gaussian random fields with known means and covariance functions. The F, R, H and Q are first decomposed into finite series in terms of Gaussian standard random variables by the Karhunen–Loeve expansion. The hydraulic head h is then represented by a perturbation expansion, and each term in the perturbation expansion is written as the products of unknown coefficients and Gaussian standard random variables obtained from the Karhunen–Loeve expansions. A series of deterministic partial differential equations are derived from the stochastic partial differential equations. The resulting equations for uncorrelated and perfectly correlated cases are developed. The equations can be solved sequentially from low to high order by the finite element method. We examine the accuracy of the KLME approach for the groundwater flow subject to uncorrelated or perfectly correlated random inputs and study the capability of the KLME method for predicting the head variance in the presence of various spatially variable parameters. It is shown that the proposed numerical model gives accurate results at a much smaller computational cost than the Monte Carlo simulation.  相似文献   

8.
    
In this paper, the application of Backus—Gilbert’s inversion method to the potential field anomalies for evaluating gravity and magnetic inversion solutions is discussed. Errors in data and singularity of kernels in the equations result in difficulties in solving equations. The application of regularization method similar to spectral expansion method makes calculation fast and easily. To make solution stable, constraints are used, which make the spread of solutions become narrow, standard deviation become small and iterative computations of inversion become fast. Finally, the author analyses specifically two profiles of Yunchen basin and calculated the Moho interface and the Curie isotherm of these two profiles. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,13, 212–221, 1991.  相似文献   

9.
Satellite orbital data yield reliable values of low degree and order coefficients in the spherical harmonic expansion of the Earth's gravity field. The second degree coefficient yields the shape of the Earth — probably the most important single parameter in geodesy. It is crucial in the numerical evaluation of different forms of the theoretical gravity formula. The new information requires the standardization of gravity anomalies obtained from satellite gravity and terrestrial gravity data in the context of three most commonly used reference figures, e.g.,International Reference Ellipsoid, Reference Ellipsoid 1967, andEquilibrium Reference Ellipsoid. This standardization is important in the comparison and combination of satellite gravity and gravimetric data as well as the integration of surface gravity data, collected with different objectives, in a single reference system.Examination of the nature of satellite gravity anomalies aids in the geophysical and geodetic interpretation of these anomalies in terms of the tectonic features of the Earth and the structure of the Earth's crust and mantle. Satellite results also make it possible to compute the Potsdam correction and Earth's equatorial radius from the satellite-determined geopotential. They enable the decomposition of the total observed gravity anomaly into components of geophysical interest. They also make it possible to study the temporal variations of the geogravity field. In addition, satellite results make significant contributions in the prediction of gravity in unsurveyed areas, as well as in providing a check on marine gravity profiles.On leave from University of Hawaii, Honolulu.  相似文献   

10.
A methodology for improving geopotential models has been developed. Theoretical relations have been derived converting coefficients in harmonic expansions for radial distortions due to geopotential models into geopotential Stokes coefficients. Terms of the order of 10 –10 in magnitude have been retained.  相似文献   

11.
    
This paper describes synthetically the seismic activity, deep and shallow structures and rock dynamic features in and near Chaoyang—Yixian region. It is supposed that there is a low velocity layer in middle crust and the three-layered crustal velocities are all lower than that in both sides of the region. There exists uplifts of upper mantle and asthenosphere-low resistance layer. It is also studied the composition of matter of three-layered crust, low velocity layer, upper mantle and asthenosphere. In the end the direct relations between the deep and shallow structure, composition and the seismic activity and new activities of faults in this region are discussed. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, 180–186, 1992.  相似文献   

12.
黑水─泉州地学断面的重磁解释   总被引:9,自引:1,他引:9       下载免费PDF全文
讨论华南黑水─泉州地学断面的重磁解释。在解释中除应用常规的2.5维重磁异常反演外,还采用等密度线算法构制梯度层密度模型,用于分辨地壳密度细结构,以及计算自由地幔而深度用于分析上地幔密度的横向不均匀性。重磁模拟结果揭示了10km深度内的上地壳构造以及地壳与上地幔密度的分布。提出华南造山带以低密度上地幔为特征,它可能与上地幔的改造有关;四川盆地具有较高的上地幔密度,为未经改造的原始地幔。扬子克拉通与华南造山带的分界线与上地幔密度的分界线一致。根据布格异常、地表岩石密度和地形资料的综合分析,圈定出反映内生成矿作用深部标志的密度倒转区,可作为进一步找矿的远景区。  相似文献   

13.
讨论华南黑水─泉州地学断面的重磁解释。在解释中除应用常规的2.5维重磁异常反演外,还采用等密度线算法构制梯度层密度模型,用于分辨地壳密度细结构,以及计算自由地幔而深度用于分析上地幔密度的横向不均匀性。重磁模拟结果揭示了10km深度内的上地壳构造以及地壳与上地幔密度的分布。提出华南造山带以低密度上地幔为特征,它可能与上地幔的改造有关;四川盆地具有较高的上地幔密度,为未经改造的原始地幔。扬子克拉通与华南造山带的分界线与上地幔密度的分界线一致。根据布格异常、地表岩石密度和地形资料的综合分析,圈定出反映内生成矿作用深部标志的密度倒转区,可作为进一步找矿的远景区。  相似文献   

14.
The source parameters of the Bohai Sea earthquake, July 18, 1969 and Yongshan, Yunnan earthquake, May 11, 1974 were determined by full — wave theory synthetic seismograms of teleseismic P waves. P+pP+sP wereform were calculated with WKBJ approximation and real integral paths. One — dimensional unilateral, finite propagation source was also considered. By trail — and — error in comparing the theoretical seismograms with the observational ones of WWSSN stations, the source parameters were obtained as follow: for Bohai earthquake, φ=195°, δ=85°, λ=65°,M o=0.9×1019Nm,L=59.9km.V R=3.5km/s, ∧ R =160°; for Yongshan earthquake, φ=240°, δ=80°, ∧=150°,M o=1.3×1018Nm,L=48.8km,V R=3km/s, ∧ R =−10°, where φ is strike, δ dip angle, λ slip angle,M o seismic moment,L rupture length,V R rupture propagation speed. As III type fractures the faulting propagated along the fault planes, and ∧ R is the angle from the strike to the propagation direction. Yongshan earthquake showed complexity in its focal process, having four sub—ruptures during the first 60 seconds. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,13, 1–8, 1991.  相似文献   

15.
Seismotectonic characteristics and its relationships with crustal structure have been analyzed in the lower Yangzi—South Yellow Sea area. The finite element method is employed to evaluate the stress-strain status of the lithosphere, and the dynamic origin of earthquakes is discussed. The moderate-weak earthquake division is tectonically controlled by three first-degree faults in the Hangzhou bay—Qinling, Tancheng—Lujiang, and the Yangzi River mouth—Jizhou island. The earthquake frequency is higher than 70% in the major hypocentral layer of the crust at a depth of 5 to 15 km of which the highest frequency particularly emerges at a depth of 10 to 15 km, and generally, the depth ranges from 5 to 20 km in the predominant hypocentral layer. The hypocentral layer is superimposed in the crustal magnetosphere with the mid-crustal low density layer. The results from the finite element analysis show that the maximum horizontal displacements appear in the hypocentral layer of the crust, and that the radial hypocentral zones on the flanks of the anomalous mantle, accompanied by the faults or fractured zones, correspond to the gradient zones of the major principal stresses and strains varying within the lithosphere. Therefore, we could consider the mechanism of the decoupling-drift of the lithosphere and the crustal sliding or detachment, from the continent to the sea, as a main dynamogenesis of the earthquakes in the area studied. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, 164–171, 1992. This research was supported by the China National Post-Doctoral Research Foundation in part. Some contents on the aeromagnetic anomalies and their mathematical processes are deleted in revision.  相似文献   

16.
This paper introduces how the ratioR of the characteristic stiffness of rock samplevs. the stiffness of testing machines would influence the rupturing process and the acoustic emission (AE) on the part of the tested rock samples. Result of the experiment shows: WhenR>0.20, the rock sample would rupture abruptly; whereas whenR<0.20, the rock samples would rupture slowly. When the samples rupture abruptly, the time-dependent variation of the AE rate takes such a pattern:peak value—stable low values—rises to the maximum value (concentration)—drops back to the minimum value (quiescence)—(rises again)—ruptures. Moreover, smallerR-value tends to be associated with longer quiescence and vice versa. WhenR>1.50, no pre-failure quiescence is detected. When the rock samples rupture slowly, the variation pattern of the AE rate (after the stress has increased to more than 50% of the rupturing stress) is as the following:stable low (or high) values—rises (or drops) to its maximum (or minimum) values and then continues for some time—ruptures. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,13, 223–233, 1991. This study is supported by the Chinese Joint Seismological Science Foundation.  相似文献   

17.
The ancient tectonic stress field in North China during 16–17th centuries were recovered by studying seismogenic faults of four great earthquakes. Three of them are dip slip events, the direction of the maximum principal stress is vertical, and that of the minimum principal stress is in the NW—SE direction and nearly horizontal tensile stress. Another earthquake is a complicated one which includes thrust and dip-slip activities. The above-stated character is quite different from that of present stress field, it is inferred that the stress field has significantly changed since 16th century, the main stress axis revolved an angle of 90 degrees nearly. The mantle upheaval in the faulted basins in North China during 16–17th centuries may cause the tensile stress field and a series of great earthquakes. The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, 144–148, 1992.  相似文献   

18.
Assessments of pyroclastic flow (PF) hazards are commonly based on mapping of PF and surge deposits and estimations of inundation limits, and/or computer models of varying degrees of sophistication. In volcanic crises a PF hazard map may be sorely needed, but limited time, exposures, or safety aspects may preclude fieldwork, and insufficient time or baseline data may be available for reliable dynamic simulations. We have developed a statistically constrained simulation model for block-and-ash type PFs to estimate potential areas of inundation by adapting methodology from Iverson et al. (Geol Soc America Bull 110:972–984, 1998) for lahars. The predictive equations for block-and-ash PFs are calibrated with data from several volcanoes and given by A = (0.05 to 0.1)V 2/3, B = (35 to 40)V 2/3, where A is cross-sectional area of inundation, B is planimetric area and V is deposit volume. The proportionality coefficients were obtained from regression analyses and comparison of simulations to mapped deposits. The method embeds the predictive equations in a GIS program coupled with DEM topography, using the LAHARZ program of Schilling (1998). Although the method is objective and reproducible, any PF hazard zone so computed should be considered as an approximate guide only, due to uncertainties on the coefficients applicable to individual PFs, the authenticity of DEM details, and the volume of future collapses. The statistical uncertainty of the predictive equations, which imply a factor of two or more in predicting A or B for a specified V, is superposed on the uncertainty of forecasting V for the next PF to descend a particular valley. Multiple inundation zones, produced by simulations using a selected range of volumes, partly accommodate these uncertainties. The resulting maps show graphically that PF inundation potentials are highest nearest volcano sources and along valley thalwegs, and diminish with distance from source and lateral distance from thalweg. The model does not explicitly consider dynamic behavior, which can be important. Ash-cloud surge impact limits must be extended beyond PF hazard zones and we provide several approaches to do this. The method has been used to supply PF and surge hazard maps in two crises: Merapi 2006; and Montserrat 2006–2007.  相似文献   

19.
The non-hydrostatic part of the second zonal harmonic term has been included in the Indian gravity anomaly. The interpretation of the potential, gravity and deflection of the vertical has been produced by a new method. The depth of the source is 580 km and the solution satisfies the temperature gradient of 1°K/km. The ratio Δ Vpp > 0 shows the thermal nature of the density distribution near 670 km.  相似文献   

20.
Large-scale zonal flow driven across submarine topography establishes standing Rossby waves. In the presence of stratification, the wave pattern can be represented by barotropic and baroclinic Rossby waves of mixed planetary topographic nature, which are locked to the topography. In the balance of momentum, the wave pattern manifests itself as topographic formstress. This wave-induced formstress has the net effect of braking the flow and reducing the zonal transport. Locally, it may lead to acceleration, and the parts induced by the barotropic and baroclinic waves may have opposing effects. This flow regime occurs in the circumpolar flow around Antarctica. The different roles that the wave-induced formstress plays in homogeneous and stratified flows through a zonal channel are analyzed with the BARBI (BARotropic-Baroclinic-Interaction ocean model, Olbers and Eden, J Phys Oceanogr 33:2719–2737, 2003) model. It is used in complete form and in a low-order version to clarify the different regimes. It is shown that the barotropic formstress arises by topographic locking due to viscous friction and the baroclinic one due to eddy-induced density advection. For the sinusoidal topography used in this study, the transport obeys a law in which friction and wave-induced formstress act as additive resistances, and windstress, the effect of Ekman pumping on the density stratification, and the buoyancy forcing (diapycnal mixing of the stratified water column) of the potential energy stored in the stratification act as additive forcing functions. The dependence of the resistance on the system parameters (lateral viscosity ε, lateral diffusivity κ of eddy density advection, Rossby radius λ, and topography height δ) as well as the dependence of transport on the forcing functions are determined. While the current intensity in a channel with homogeneous density decreases from the viscous flat bottom case in an inverse quadratic law ~δ –2 with increasing topography height and always depends on ε, a stratified system runs into a saturated state in which the transport becomes independent of δ and ε and is determined by the density diffusivity κ rather than the viscosity: κ/λ 2 acts as a vertical eddy viscosity, and the transport is λ 2/κ times the applied forcing. Critical values for the topographic heights in these regimes are identified.  相似文献   

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