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1.
大地电磁测深二维反演方法求解复杂电性结构问题的适应性研究 总被引：3，自引：1，他引：2
为探讨二维反演方法在三维电性结构中的适应性问题,本研究中设计了一系列的二维/三维正演模型进行实验计算,分析了三维高阻/低阻异常体对模型响应的畸变作用,并从反演模式选择和数据旋转方向两个方面进行模型二维反演的对比分析,与三维反演的结果进行了比较,最后采用了实测数据进一步进行了二维和三维反演的比较实验.实验和研究结果表明,在剖面选择方面,在剖面方向与垂直主构造方向相差不大的情况下,截取剖面方向,将电性主轴旋转到垂直剖面方向的二维反演结果与垂直主构造方向的反演结果都可以较好地还原正演模型,在大的构造的反映上并无太大差异.在地下为二维或近三维条件时,正演模型的主要结构都可以较好地被二维和三维反演解析出来.二维的反演结果可能甚至会比三维的反演结果的边界更清晰,更精确.然而,对于具有较强的三维结构的模型而言,其二维反演结果与原始模型可能仍然存在较大差异,其中TM+TP或TM模式的二维反演结果相对更接近原始模型,而TE模式的结果往往会有较大误差,需要在解释时特别注意以免得出错误结论. 相似文献
2.
Application of 2D magnetotelluric methods in a geological complex area, Xinjiang, China 总被引：2，自引：0，他引：2
Qibin Xiao Xinping CaiGuanghe Liang Xingwang XuBaolin Zhang 《Journal of Applied Geophysics》2011,75(1):19-30
Magnetotelluric (MT) data along two profiles were collected in Tulargen Cu-Ni mining area, Xinjiang, China. The MT profiles, crossing the known ore-bearing magmatic body, are interpreted to have further understanding of the ore-bearing magmatic bodies' stretch and shape in depth, and to evaluate the prospect in the mining area. The values of phase sensitivity skewness indicate a contaminated two-dimensional (2D) structure (there exist local three-dimensional (3D) structures at shallow level) over 3D structures. G-B decomposition of the impedance tensors indicates the dominant geoelectrical strike in survey area is in East-West direction. To obtain reliable electrical structures, four different 2D inversion codes as REBOCC, NLCG, OCCAM, and ABIC are adopted, inversions of a synthetic 3D model using these codes indicate TM data are more suitable to invert the electrical structures along the profiles in Tulargen Cu-Ni mining area, while TE and TE + TM inversions can be used to verify the transverse variation of electrical structures at shallow level. The 2D electrical structures show high-resistivity basement covered by relatively low-resistivity strata in the mining area, the conductive anomalies are imbedded in the upper covers. The known ore-bearing magmatic body is coincided with the positions of two conductive anomalies in both profiles at shallow level; its extension at depth is deduced according to the shapes of the anomalies. Other conductive anomalies, isolated and existing only at limited depth as the known ore-bearing magmatic body, are presumed of good prospect. 相似文献
3.
针对大地电磁二维反演中TE、TM极化模式的选择问题,设计了多个二维、三维模型进行了正演计算,从数据对比和反演结果对比两方面入手,分析研究了三维模型和二维模型响应数据的差异、反演中极化模式的选择、以及三维模型数据的二维反演近似等问题.研究结果表明:在三维模型条件下,利用二维模型进行反演时,TE模式对模型的二维的近似程度要求远高于TM模式;当三维结构影响较明显时,利用TM模式数据进行二维反演比利用TE模式或利用TE+TM模式联合反演都更合理,反演结果中的虚假结构明显减少;对于TM模式,相位受三维畸变影响较小,视电阻率较大,所以二维反演中可适当加大相位的权;对于实测数据的二维反演,应优先考虑采用TM模式数据进行二维反演,其次是TM+TE模式,一般不要单独采用TE模式. 相似文献
4.
Mohamed Abdelzaher Jun Nishijima Hakim Saibi Gad El-Qady Usama Massoud Mamdouh Soliman Abdellatif Younis Sachio Ehara 《Pure and Applied Geophysics》2012,169(9):1679-1692
Magnetotelluric (MT) soundings and gravity methods were employed to study the deep freshwater aquifer in the area north of Abo Zenema city on the eastern side of the Gulf of Suez, Egypt. Seven MT sites and 48 gravity stations were surveyed along northeast–southwest profiles as close as possible to a line perpendicular to the coast of the Gulf of Suez. The MT survey was conducted using high and low frequencies to investigate shallow and deep areas, respectively. One-dimensional inversion was conducted using a heuristic inversion scheme of the Bostick algorithm. The MT data were also inverted with a 2-D smooth model inversion routine using the nonlinear conjugate gradient method to infer variation in vertical and lateral resistivity inside the Earth. A 100-Ohm-m homogeneous half-space initial model was used to invert the TE mode data only. Then, the inverted model obtained from the TE mode data was used as an initial model for inversion of the TM mode data. The inverted model thus obtained from the TM mode data inversion was used as an initial model for the inversion of the joint TE and TM responses. Two-dimensional (2-D) forward modeling of the gravity data was conducted using the 2-D polygon method of Talwani’s algorithm for an arbitrarily shaped body and was based on the subsurface information from the MT survey and the available information about the geological structure of the study area. This method enabled us to obtain the basement structure of the coastal aquifer in the study area. The results from the analysis and the interpretation of MT and gravity data were used to detect and delineate the groundwater coastal aquifer in the study area. 相似文献
5.
岷山隆起带与西秦岭构造带中段位于青藏高原物质东向流动的必经之处,又是南北地震带的组成部分和GPS速度场非连续性衰减和转换的关键部位,其地壳结构及地壳变形机制受到国内外地质地球物理学家的广泛关注,了解研究区深部细结构及主要边界断裂空间展布特征,对青藏高原隆升机制及中强地震孕震构造的研究有重要意义.本文依托分别横跨岷山隆起带及西秦岭构造带中段的两条大地电磁剖面(SG-WQL-L1与SG-WQL-L2)小点距观测数据,采用大地电磁相位张量分解技术对两条剖面上各个测点的电性走向、二维偏离度进行计算分析,根据分析结果对原始数据进行主轴方位角校正处理,进一步采用NLCG(非线性共轭梯度)二维反演方法开展TE与TM模式的相位和电阻率联合反演,获取沿剖面方向30 km以浅的电阻率结构模型,并完成了地质地球物理综合解释.两条大地电磁剖面勘探成果揭示出,马尔康地块中上地壳发育的壳内低阻层与峨山隆起上地壳低阻体在深部交汇,岷江断裂带与虎牙断裂带受控于马尔康地块与岷山隆起带上地壳底部的滑脱面,滑脱面呈现往东角度逐渐变陡峭的趋势且在岷江附近出现"断坡"构造,历史强震震源深度显示虎牙断裂为岷山隆起带新生代强震的发震断裂;西秦岭构造带中段中上地壳沿剖面方向表现为横向分块、纵向分层的电性结构特征,中地壳12~25 km左右发育厚度不等的壳内低阻层,壳内低阻层多与研究区次级地块的边界断裂在深部交汇,次级地块以及区分次级地块的活动断裂带可能是GPS速度场在研究区呈现非连续性的递减并伴随方向转换的构造成因;青藏高原内部的软流圈物质向NE和SSE流动,驱动巴颜喀拉地块东缘上地壳沿中上地壳低阻层东向运移,受到摩天岭高阻地块的阻挡作用,软弱的岷山隆起带发生地壳褶皱变形并向东逆冲推覆从而形成高耸的岷山山脉,岷江断裂与虎牙断裂的左旋运动加速了岷山的隆起. 相似文献
6.
穿过郯庐断裂带中段（沂沭断裂带,36°N）所做的大地电磁测深（MT）剖面长约150km.使用Robust技术和远参考道大地电磁方法处理观测数据.通过分析视电阻率、阻抗相位、Swift二维偏离度和区域走向,定性确定测区的电性结构.二维反演解释中选择非线性共轭梯度（NLCG）方法,使用TE、TM两种模式资料联合反演,沿剖面的二维电性结构显示：自西向东,鲁西隆起、郯庐断裂带、胶莱坳陷及鲁东隆起4个电性区块分别对应,鲁东和鲁西隆起区为高阻,郯庐断裂带电性结构复杂,高、低阻相间,胶莱坳陷为低阻（高导）区.沿MT剖面附近曾发生3个地震,其震源区处在电性变化剧烈部位,并在震源区附近存在高导体. 相似文献
7.
M. Bastani A. Savvaidis L.B. Pedersen T. Kalscheuer 《Journal of Applied Geophysics》2011,75(2):180-195
In order to gain a better understanding of the geometry of surface faults, five Controlled Source/Radio Magnetotelluric (CSRMT) profiles were measured across the Volvi basin, 45 km northeast of the city of Thessaloniki in Greece. The data were collected in two frequency ranges: a) 1–12.5 kHz using a remotely controlled double horizontal magnetic dipole transmitter (CSAMT measurements), and b) 15–250 kHz using the signal from distant radio transmitters (RMT measurements). The transition from the RMT band to the CSAMT band was smooth and continuous allowing us to combine both datasets for plane-wave modeling. The surface geology shows a predominantly 2D structure, and therefore we planned the survey into profiles perpendicular to the geological strike. We have used a 2D interpretation tool to model the data in TE, TM, TE + TM and determinant modes. Using a 4% error floor on the impedance, 2D resistivity models from inversion of the determinant data provide lower RMS data fits (4.2 and 1.2 for resistivity and phase, respectively) compared to the combined TE + TM data (4.4, 2.8, overall resistivity and phase, respectively). 2D inversion of the measured tensor data shows a sharp change in the depth to the top of resistive gneiss–schist basement that is overlain by a less resistive overburden at southern basin flanks. The change in depth to the bedrock is clearly seen in all 2D models along the measured profiles suggesting the existence of normal faults with strike directions of NE–SW to E–W. The 2D electrical resistivity models suggest that the bedrock deepens towards south-west. The resistivity models are also compared with the existing borehole information in the area and show a reasonable correlation. For example the sharp change of depth to the bedrock towards the center of the basin as seen in the resistivity models are also confirmed by the borehole data. 相似文献
8.
María de los Ángeles García Juanatey Juliane Hübert Ari Tryggvason Laust B. Pedersen 《Geophysical Prospecting》2013,61(1):200-219
New magnetotelluric (MT) data from two perpendicular profiles in the Kristineberg area, northern Sweden, were analysed and modelled. In the Skellefte Ore District, the Kristineberg volcanic hosted massive sulphide (VHMS) deposit mine is one of the largest and deepest (1250 m). Seventeen broadband magnetotelluric stations were installed along two existing seismic reflection lines. The profiles were 6 and 12 km long with 500 m and 1 km site spacing, respectively. The obtained MT transfer functions in the period range of 0.0015–200 s are of fairly good quality. Detailed strike and dimensionality analysis reveal consistent but period dependent, strike directions, indicating a change in the geoelectrical strike with depth. From the two‐dimensional inversion of the determinant of the impedance tensor, two stable conductivity models with good data fit were obtained. The addition of seismic reflection information from the co‐located survey, improved the data fit of one of them. Extensive sensitivity analyses helped to delineate the well resolved regions of the models and to determine the position of pronounced boundaries. The results are in good agreement with previous studies, especially regarding the presence of a deep conductor interpreted as a structural basement to the district. They also reveal with more detail the configuration of the main geological units of the Skellefte Ore District, especially of the ore bearing volcanic rocks and the embedded alteration zones. 相似文献
9.
本文对位于青藏高原东缘川滇构造区的贡山一绥江大地电磁测深(MT)剖面数据进行反演,获得沿剖面的深部电性结构,为研究喜马拉雅东构造结、川滇菱形地块与华南地块的构造变形特征、壳幔耦合关系、地块间接触关系以及相互作用等问题,提供电性结构的依据.研究发现:(1)电性结构揭示澜沧江断裂带和小金河断裂带为深大断裂带,控制着研究区的深部结构特征和形变机制;(2)澜沧江断裂带和金沙江断裂带之间的高阻体,可能是扬子古地块的残留部分;小金河断裂带和安宁河断裂带之间的高阻体,则是峨眉山大火山省喷发形成的冕宁一越西杂岩带;(3)在滇西地块、川滇地块和大凉山地块均存在低阻层,它们的介质属性有所不同,滇西地块下的低阻层"疑似"高热状态的岩浆囊,主要由缅甸弧向东俯冲运动引起的,中上地壳的高热状态使地块的活动性增强;川滇地块内部的壳内低阻层的成因为:理塘断裂带和小金河断裂带之间的地表低阻层由破碎带充水所致,而金沙江断裂带和理塘断裂带之间的中地壳低阻层可能是由局部熔融物质或含盐流体导致的,其为壳内物质运移的通道.从而在地下物质发生大规模走滑运动的过程中起到引导作用;川滇地块东部和大凉山地块西部的壳内低阻层可能与地慢物质的上涌有关;马边断裂带附近的低阻体可能与破碎带变宽和破碎带内的流体有关. 相似文献
10.
Deep structure of the northeastern margin of the Parnaiba Basin, Brazil, from magnetotelluric imaging 总被引：1，自引：0，他引：1
The magnetotelluric (MT) method has been applied to the determination of the deep resistivity structure of the northeastern margin of the Parnaiba Basin. Transient electromagnetic (TEM) and MT data were collected in early 1999 along a 95 km long N–S line, extending from the coast across the projected subcrop position of a discontinuous fault found to the west of the study area that is believed to be a possible basin‐bounding fault. The MT data were processed to yield the TE‐ and TM‐mode responses and then corrected for static shift using central‐loop and single‐loop TEM data, respectively. Regularized 2D MT inversion was subsequently undertaken using a structured initial model with the near‐surface constrained by TEM inversion results. As a consistency check, we performed another set of 2D inversions using different smooth initial models. The various optimal 2D inversion models show clearly the presence of a major basement trough, over 2 km deep, located about 70 km from the coast. We interpret it as possibly marking the main basin margin and suggest that it may have implications for groundwater resource development in the area. 相似文献
11.
西秦岭造山带与南北地震构造带接触区是中国大陆最重要的南北向和东西向构造转化的接合部位之一.本文介绍了分别位于该区106°E东、西两侧的LMS-L3和DBS-L1两条大地电磁剖面的探测结果,两条剖面分别跨过了龙门山构造带东北段的青川段和宁强段.采用大地电磁相位张量分解技术对两条剖面上各测点的电性走向、二维偏离度等进行了计算和分析,采用NLCG二维反演方法对TE+TM模式的视电阻率和阻抗相位数据进行了二维联合反演.反演得到二维电性结构,在经度106°西侧LMS-L3剖面的深部电性结构自北向南揭示出,西秦岭北缘、成县盆地北缘、康县（即勉略构造带）和平武-青川断裂带都表现为明显的电性梯度带,深部延伸可达几十公里;西秦岭造山带、碧口地块与龙门山构造带东北段3个构造单元整体表现为高电阻体、呈现往南叠合且角度逐渐变陡的趋势.在106°E西侧西秦岭造山带区域的深部存在壳内低阻层,而东侧区域表现为高电阻体,深部电性结构在106°E东、西两侧的差异与该区深部速度结构特征一致,东、西两侧深部结构差异可能是该区中强地震分布差异的深层原因.LMS-L3和DBS-L1两条剖面南段的深部电性结构图像揭示出龙门山构造带东北部的青川段和宁强段内的平武-青川断裂带具有明显不同的深部结构特征,平武-青川断裂带在青川段为明显的电性梯度带,在宁强段不再表现为电性梯度带,而是完整的高电阻块体.汶川强余震向东北发展止于青川青木川附近,与平武-青川断裂带延伸深度和向北东方向的延伸长度密切相关,同时高电阻块体的宁强段对汶川强余震东北发展起到了阻挡作用. 相似文献
12.
Introduction Ready and Renkin (1971) were the first to make the research on anisotropy problems in magnetotellurics (MT). The progress in the research is not evident because it is more complex and difficult than isotropic problems. Now, the one-dimensional (1D) anisotropy problems in MT have been well solved, while for the two-dimensional (2D) cases, the numerical solutions have only been obtained for some particular conditions (Ready and Renkin, 1975). As to the three-dimensional (3D) ani… 相似文献
13.
局部畸变问题曾经困扰大地电磁资料反演解释几十年,大地电磁三维数值模拟技术的发展为剖析局部畸变特点和得到可靠的反演成像结果提供了技术基础。本文采用三维数值模拟成像方法对典型三维局部畸变模型进行模拟分析。三维数值模拟结果显示:电场分量垂直电性分界面的极化模式视电阻率曲线(对应二维情况下TM模式)在穿越低阻异常体界面时,曲线会先上移后下移,而在穿越高阻异常体界面时,曲线会先下移后上移,这与电性分界面处积累面电荷产生的二次电场有关。三维模型中XY模式、YX模式视电阻率和相位在三维异常体附近的水平变化是呈现近似垂向对称的,该现象与电场垂直跨越电性界面时视电阻率的变化规律是吻合的,当测线分别沿X方向和Y方向展布时,三维情况下的XY和YX模式分别对应二维情况下的TM模式。低阻小异常体对区域构造响应的畸变影响比高阻小异常体要严重。低阻小异常体对二维区域响应的两种极化模式视电阻率和相位都有非常明显的畸变影响,相比较而言对TE模式的畸变要大于TM模式,因此我们在做二维反演解释时,可优先考虑拟合TM模式数据。位于小异常体中心上方测点的三维畸变响应虽然与对应真实二维区域响应的差异比较大,但可以等效于某种二维模型响应,这种由局部畸变造成的假二维响应在实际野外数据的解释中是需要注意的。 相似文献
14.
Three‐dimensional modelling of magnetotelluric data to image Sehqanat hydrocarbon reservoir in southwestern Iran 
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下载免费PDF全文 A detailed magnetotelluric survey was conducted in 2013 in the Sehqanat oil field, southwestern Iran to map the geoelectrical structures of the sedimentary Zagros zone, particularly the boundary between the Gachsaran Formation acting as cap rock and the Asmari Formation as the reservoir. According to the electrical well logs, a large resistivity contrast exists between the two formations. The Gachsaran Formation is formed by tens to hundreds of metres of evaporites and it is highly conductive (ca. 1 Ωm–10 Ωm), and the Asmari Formation consists of dense carbonates, which are considerably more resistive (more than 100 Ωm). Broadband magnetotelluric data were collected along five southwest–northeast directed parallel lines with more than 600 stations crossing the main geological trend. Although dimensionality and strike analysis of the magnetotelluric transfer functions showed that overall they satisfied local 2D conditions, there were also strong 3D conditions found in some of the sites. Therefore, in order to obtain a more reliable image of the resistivity distribution in the Sehqanat oil field, in addition to standard 2D inversion, we investigated to what extent 3D inversion of the data was feasible and what improvements in the resistivity image could be obtained. The 2D inversion models using the determinant average of the impedance tensor depict the main resistivity structures well, whereas the estimated 3D model shows significantly more details although problems were encountered in fitting the data with the latter. Both approaches resolved the Gachsaran–Asmari transition from high conductivity to moderate conductivity. The well‐known Sehqanat anticline could also be delineated throughout the 2D and 3D resistivity models as a resistive dome‐shaped body in the middle parts of the magnetotelluric profiles. 相似文献
15.
稀疏测线大地电磁资料三维反演研究:合成算例(英文) 总被引：2，自引：1，他引：1
受勘探成本和工区环境等因素的影响,当前大多数大地电磁实际工作采取布置稀疏测线采集数据和使用二维反演方法解释这些稀疏测线数据的方式。然而,二维反演方法在解释三维地电构造数据时存在局限性,有时甚至做出错误的地质解释。本文尝试了使用三维反演方法对大地电磁稀疏测线数据进行反演解释。使用大地电磁全信息资料三维共轭梯度反演程序对理论模型合成稀疏测线数据进行了三维反演。结果表明:这种反演方案是可行与有效的。同时,我们发现在不同数据的三维反演结果中,四个张量阻抗元素和两个倾子数据同时反演的结果相对更为准确,更接近理论模型。 相似文献
16.
本文采用反射映像（即U/D成像）原理对大地电磁资料进行成像,将地面观测的波场分解成上行波和下行波,并分别向下延拓,利用上、下行波的时间一致性原理确定地下电性界面的位置.对TE和TM模式的MT响应分别处理可以得到两个深度剖面,两剖面的一致性便为实际反射界面的最佳估计.理论和实际资料的计算表明,MT偏移技术是比较有效的,它可获得地下界面直观的映像.和常规MT反演方法相比较,该方法具有算法简单等优点,并且还能获得表示地下地质构造真实映像的MT深度剖面. 相似文献
17.
Derecke Palmer 《Geophysical Prospecting》2010,58(2):203-218
Non‐uniqueness occurs with the 1D parametrization of refraction traveltime graphs in the vertical dimension and with the 2D lateral resolution of individual layers in the horizontal dimension. The most common source of non‐uniqueness is the inversion algorithm used to generate the starting model. This study applies 1D, 1.5D and 2D inversion algorithms to traveltime data for a syncline (2D) model, in order to generate starting models for wave path eikonal traveltime tomography. The 1D tau‐p algorithm produced a tomogram with an anticline rather than a syncline and an artefact with a high seismic velocity. The 2D generalized reciprocal method generated tomograms that accurately reproduced the syncline, together with narrow regions at the thalweg with seismic velocities that are less than and greater than the true seismic velocities as well as the true values. It is concluded that 2D inversion algorithms, which explicitly identify forward and reverse traveltime data, are required to generate useful starting models in the near‐surface where irregular refractors are common. The most likely tomogram can be selected as either the simplest model or with a priori information, such as head wave amplitudes. The determination of vertical velocity functions within individual layers is also subject to non‐uniqueness. Depths computed with vertical velocity gradients, which are the default with many tomography programs, are generally 50% greater than those computed with constant velocities for the same traveltime data. The average vertical velocity provides a more accurate measure of depth estimates, where it can be derived. Non‐uniqueness is a fundamental reality with the inversion of all near‐surface seismic refraction data. Unless specific measures are taken to explicitly address non‐uniqueness, then the production of a single refraction tomogram, which fits the traveltime data to sufficient accuracy, does not necessarily demonstrate that the result is either ‘correct’ or the most probable. 相似文献
18.
Mahmoud Mekkawi Pierre-Andr Schnegg Tarek Arafa-Hamed Essam Elathy 《Earth and Planetary Science Letters》2005,240(3-4):764-773
In this work, we use the magnetotelluric (MT) method to detect geoelectrical conductivity anomalies in the Earth's crust and link them to local seismic activity. This application affords the unusual opportunity to study the percolation of water from a lake into a fault system and its effect on the induced seismicity. MT measurements were carried out in the period range 0.0046–420 s at nine sites along a 15 km-long North–South profile crossing the Kalabsha Fault, on the western bank of Lake Aswan. Data were analysed by 2D simultaneous inversion of both polarisations. The resulting model is compared with the local seismicity map and reveals the conductive signature of the fault, as well as geological and tectonic stresses prevailing in the Aswan area. Our MT investigations show the following features:
The measured MT strike aligns with the seismic epicentre axis corresponding to the Kalabsha Fault.
While crossing the Fault, enhanced conductivity is found down to depths of 5 km on a 1–2 km profile segment.
At mid-crustal depths (20 km), a very high conductive body is found to coincide with the main seismic cluster in the Aswan area.
These observations indicate that seismic activity and high electrical conductivity are related. The link between them is the presence of crustal fluids which are presumably the cause of the high conductivity observed. Their presence is also required to trigger the observed seismicity. In addition, we explain the lower conductivity of the local upper crust in terms of stress-modulated rock porosity. We believe that these results are of general significance, as they could explain the mid-crustal seismicity of tectonically active zones. 相似文献
19.
本文利用大地电磁测深数据,对穿过兰坪—思茅地块和川滇菱形地块以及进入扬子地块的云南兰坪—贵州贵阳大地电磁测深剖面展开了深部电性结构研究.采用大地电磁数据处理分析以及反演技术,对观测资料进行了由定性到定量全面地分析,通过二维非线性共轭梯度反演得到了沿剖面的较为详细的地壳上地幔电性结构,结合其他地质和地球物理资料的分析,对该剖面的二维电性结构进行解释,确定了主要断裂带和边界带的位置以及深部延伸情况,同时确定了壳内低阻层的分布位置,最后进行了区域动力学和孕震构造环境的探讨.研究表明:剖面壳幔电性结构分块性特征与区域地质构造分布特征基本一致,不同地块的电性结构存在显著差异,其中川滇菱形地块的结构相对复杂,上地壳的电性结构为高低阻相间分布特征,电阻率的突变带与地表断裂具有很好的对应关系;兰坪—思茅地块存在中上地壳低阻层,川滇菱形地块中西部存在下地壳低阻层,川滇菱形地块东部和华南地块西部存在中上地壳的低阻层;川滇菱形地块中部攀枝花附近的低阻层埋深最深,而华南地块西部会泽附近的低阻层埋深则最浅;兰坪—思茅地块和川滇菱形地块的中下地壳的低阻层可能与青藏高原物质的东南逃逸有关;华南块体的宣威以东的下地壳不存在低阻层,华南块体下地壳和上地幔的电阻率较高;攀枝花附近的高阻体可能是峨眉山玄武岩喷发导致底侵作用及幔源物质上侵的结果. 相似文献
20.
横过松嫩地块东缘和佳木斯地块西缘的大地电磁测深剖面揭示了两块体结合带附近的深部电性结构.本文对剖面测点做了标准化数据处理,并对二维偏离度、构造走向进行了计算和分析,采用非线性共轭梯度(NLCG)二维反演方法对TM模式的数据进行了反演,获得了该剖面的地壳、上地幔电性结构模型,划分出三个典型构造单元:松嫩地块东缘、碰撞拼合带和佳木斯地块西缘.研究结果表明,研究区上地壳基本呈高阻特征,可能为岩浆岩,代表其经历了多期次岩浆作用,而松嫩地块东缘和佳木斯地块西缘的中下地壳的高导体可能与地幔物质的上涌有关;拼合带下方存在西倾的高导体和高阻体,可能是佳木斯地块向西俯冲到松嫩地块下方的构造遗迹;研究区可能发生了拆沉作用,与之伴随的地幔物质上涌可能是后期伸展作用的一个动力. 相似文献