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71.
P. Yu. Pushkarev T. Ernst J. Jankowski W. Jozwiak M. Lewandowski K. Nowozynski V. Yu. Semenov 《Geophysical Journal International》2007,169(3):926-940
The deep resistivity structure was estimated along a 400-km profile in central Poland crossing the Malopolska Massif (MM), the Lysogory Unit (LU), the Trans-European Suture Zone (TESZ) and ending at the East European Craton (EEC). Magnetotelluric transfer functions, corresponding to 20 sites, were supplemented by magnetovariational responses obtained at the geomagnetic observatories situated at the same tectonic units. Such a combination made it possible to extend the initial period range, which is from fractions of a second to several hours, up to months in order to reliably cover crustal and upper-mantle depths. The geoelectrical structures, revealed using 2-D inversions, do not contradict the known features of the lithosphere structure determined using seismic and gravity data along the profile.
The subsurface conductance, varying from approximately 10 Siemens at the inner part of the EEC to about 600 Siemens in the TESZ, is produced by sediments, the deep part of which contains conductive, highly mineralized water. The existence of two crustal conductive faults at the southwest and northeast of the TESZ were established mainly by the use of induction arrows. It was also revealed that rather high mantle conductivity beneath the MM, LU and TESZ at depths of about 150–200 km contrasts with the resistive upper mantle of the EEC. This can be interpreted as the decrease of asthenosphere conductance and/or as its submersion beneath the EEC. Generally, the results confirm the idea that the TESZ forms not only specific seismic boundaries but also causes peculiar conductivity anomalies in the crust and upper mantle. 相似文献
The subsurface conductance, varying from approximately 10 Siemens at the inner part of the EEC to about 600 Siemens in the TESZ, is produced by sediments, the deep part of which contains conductive, highly mineralized water. The existence of two crustal conductive faults at the southwest and northeast of the TESZ were established mainly by the use of induction arrows. It was also revealed that rather high mantle conductivity beneath the MM, LU and TESZ at depths of about 150–200 km contrasts with the resistive upper mantle of the EEC. This can be interpreted as the decrease of asthenosphere conductance and/or as its submersion beneath the EEC. Generally, the results confirm the idea that the TESZ forms not only specific seismic boundaries but also causes peculiar conductivity anomalies in the crust and upper mantle. 相似文献
72.
An important question in seismic hazard assessments is the frequency-size and recurrence interval statistics at a point on a fault. Does a point on a fault obey the same statistics as earthquakes in a region do? This is a difficult question to answer because the number of repetitive earthquakes on a particular fault that have been observed is small. In order to overcome this difficulty we consider slip events on the creeping section of the San Andreas fault in central California. Sequences of up to 100 events are obtained from creepmeter records. We compare the statistical distribution of recurrence times with the Brownian passage-time, lognormal, and Weibull distributions and using goodness-of-fit tests find that the Weibull is the preferred distribution. We also consider the frequency–amplitude distribution of slip events. We find that the data clearly do not obey a Gutenberg–Richter distribution. Instead there is a uniform distribution of event sizes for a large fraction of events. 相似文献
73.
74.
D. R. Toomey W. S. D. Wilcock J. A. Conder D. W. Forsyth J. D. Blundy E. M. Parmentier W. C. Hammond 《Earth and Planetary Science Letters》2002,200(3-4):287-295
The mantle electromagnetic and tomography (MELT) experiment found a surprising degree of asymmetry in the mantle beneath the fast-spreading, southern East Pacific Rise (MELT Seismic Team, Science 280 (1998) 1215–1218; Forsyth et al., Science 280 (1998) 1235–1238; Toomey et al., Science 280 (1998) 1224–1227; Wolfe and Solomon, Science 280 (1998) 1230–1232; Scheirer et al., Science 280 (1998) 1221–1224; Evans et al., Science 286 (1999) 752–756). Pressure-release melting of the upwelling mantle produces magma that migrates to the surface to form a layer of new crust at the spreading center about 6 km thick (Canales et al., Science 280 (1998) 1218–1221). Seismic and electromagnetic measurements demonstrated that the distribution of this melt in the mantle is asymmetric (Forsyth et al., Science 280 (1998) 1235–1238; Toomey et al., Science 280 (1998) 1224–1227; Evans et al., Science 286 (1999) 752–756) at depths of several tens of kilometers, melt is more abundant beneath the Pacific plate to the west of the axis than beneath the Nazca plate to the east. MELT investigators attributed the asymmetry in melt and geophysical properties to several possible factors: asymmetric flow passively driven by coupling to the faster moving Pacific plate; interactions between the spreading center and hotspots of the south Pacific; an off-axis center of dynamic upwelling; and/or anomalous melting of an embedded compositional heterogeneity (MELT Seismic Team, Science 280 (1998) 1215–1218; Forsyth et al., Science 280 (1998) 1235–1238; Toomey et al., Science 280 (1998) 1224–1227; Wolfe and Solomon, Science 280 (1998) 1230–1232; Evans et al., Science 286 (1999) 752–756). Here we demonstrate that passive flow driven by asymmetric plate motion alone is not a sufficient explanation of the anomalies. Asthenospheric flow from hotspots in the Pacific superswell region back to the migrating ridge axis in conjunction with the asymmetric plate motion can create many of the observed anomalies. 相似文献
75.
P. K. Banerjee 《Journal of Earth System Science》1997,106(4):357-360
Within the Brahmani valley granulite terrane (Eastern Ghats) of Dhenkanal district, Orissa the sporadically outcropping pods
of chromite-rich serpentinite are devoid of chrome-poor enstatitite which occurs abundantly in the northern Gorumahisani greenstone
terrane as well defined units within the chromite-rich suites at Katpal, Sukinda and Boula-Nausahi, Cuttack and Keonjhar districts.
Available field evidence is compatible with a model of emplacement of these ultramafic bodies along the contact between the
two terranes in a number of stages involving soft and hard collision, subduction of Gorumahisani Group oceanic lithosphere
below the Eastern Ghats granulites followed by delamination and asthenospheric upwelling. Falsifiability tests for the model
have been indicated. 相似文献
76.
Some effects of lateral heterogeneities in the upper mantle on postglacial land uplift close to continental margins 总被引：2，自引：0，他引：2
We investigate the effects of lateral heterogeneities in the upper mantle on the calculation of postglacial land uplift. For the model calculations we use a commercial finite-element code, which enables us to solve the equations governing a layered, isotropic. incompressible, Maxwell-viscoelastic half-space with laterally varying layer thicknesses and physical properties. Following previous investigations performed by Sabadini. Yuen & Portney (1986) and Gasperini & Sabadini (1989), we extend their results using a more realistic loading history and different earth models. We then focus our attention on the question whether lateral heterogeneities in the upper mantle can be modelled correctly using a set of homogeneous earth models. To this end, a comparison of model calculations using both laterally homogeneous and heterogeneous earth models is performed.
We find that lateral heterogeneities in the upper mantle significantly influence the calculated postglacial land uplift. The resolving power of relative sea-level observations for the prescribed lateral heterogeneities used in this study is mainly focused on observations around the load margin and outside the glaciated areas, where differences in predicted land uplift between individual models are large enough to be resolved by observations.
We can qualitatively determine lateral heterogeneities in the upper mantle using a set of laterally homogeneous earth models, if the geological structure, for example a continental margin, is known. However, in order to infer the correct values of lithospheric thickness and asthenospheric viscosity, we need to use laterally heterogeneous models. 相似文献
We find that lateral heterogeneities in the upper mantle significantly influence the calculated postglacial land uplift. The resolving power of relative sea-level observations for the prescribed lateral heterogeneities used in this study is mainly focused on observations around the load margin and outside the glaciated areas, where differences in predicted land uplift between individual models are large enough to be resolved by observations.
We can qualitatively determine lateral heterogeneities in the upper mantle using a set of laterally homogeneous earth models, if the geological structure, for example a continental margin, is known. However, in order to infer the correct values of lithospheric thickness and asthenospheric viscosity, we need to use laterally heterogeneous models. 相似文献
77.
造山作用的两大类型与成因差异 总被引：3，自引：0，他引：3
根据造山作用的主要标志识别出板内造山和板缘造山两种主要造山作用类型。板块和软流圈之间不同的相对运动机制是形成不同类型造山作用的主要原因。板缘造山主要表现为岩石圈和软流圈以基本相同的运动趋势的相对运动。板内造山主要表现为同一区域内岩石圈、软流圈等不同层圈之间的不协调的相对运动。 相似文献
78.
笔者根据地震面波层析成像结果，对欧亚大陆及西太平洋岩石圈和软流圈速度结构进行了研究，发现东亚至西太平洋间存在一巨型低速异常带，结合构造地质学、地幔岩石学、地球化学及其他地球物理特性的研究，确认该区存在巨型裂谷体系。该巨型裂谷体系的岩石圈和软流圈三维Vs速度结构与太平洋洋中脊、大西洋洋中脊和印度洋洋中脊及其邻区的岩石圈和软流圈地震Vs速度结构十分相似，而与东太平洋边缘现代板块俯冲带的岩石圈与软流圈Vs速度结构有显著差异。在进一步论述该区动力学特征后认为，该巨型裂谷体系是中生代中晚期以来岩石圈整体主动伸展变形，大型裂陷盆地形成，岩石圈强烈拆沉减薄，以及软流圈物质上涌加热引起的。边缘海是在大陆裂谷系形成基础上发展起来的，主导扩张期为中渐新世至中中新世（32－13Ma），这些边缘海在17－15Ma后停止扩张，因而未能将所有边缘海和洋中脊联通。据此划分出4期构造变形动力学演化阶段，现今东亚至西太平洋间大陆裂谷、边缘海与沟弧体系是新生代中晚期以来，邻区各板块构造相互作用叠加的结果。 相似文献
79.
根据欧亚大陆及西太平洋地区58个数字地震台站约12000个长周期波形记录,挑选出4100条面波大圆传播路径,采用面波频散及波形拟合反演方法,对东亚及西太平洋边缘海地区(60°E-160°E,20°S-60°N)的地壳上地幔进行了高分辨率三维S波速度成像. 结果表明,从上地壳到70km深,在东亚东部及西太平洋边缘海地区为高速分布,西部以青藏高原为中心呈极低速分布. 自地中海经土耳其、伊朗、喜马拉雅山到缅甸、印尼群岛的特提斯汇聚碰撞带,显示为低速异常链. 从85km至250km深,在东亚东部及西太平洋边缘海,自北向南显示出一条巨型低速异常带,西部地区为高速异常分布.以东经110°E为界,东西两部分岩石圈、软流圈的结构与深部动力过程有着巨大的差异. 此界线以西主要是印度板块与欧亚板块碰撞引起的岩石圈汇聚增厚区,东部则主要是由于软流圈上涌(地幔热物质上升)引起的岩石圈拉张减薄区. 相似文献
80.