Research of the Conductive Structure of Crust and the Upper Mantle beneath the South-Central Tibetan Plateau     

叶高峰金胜  魏文博Martyn Unsworth 《中国地质大学学报(英文版)》2007,18(4):334-343

With the super-wide band magnetotelluric sounding data of the Jilong (吉隆)-Cuoqin (措勤) profile (named line 800) which was completed in 2001 and the Dingri (定日)-Cuomai (措迈) profile (named line 900) which was completed in 2004,we obtained the strike direction of each MT station by strike analysis,then traced profiles that were perpendicular to the main strike direction,and finally obtained the resistivity model of each profile by nonlinear conjugate gradients (NLCG) inversion. With these two models,we described the resistivity structure features of the crust and the upper mantle of the center-southern Tibetan plateau and its relationship with Yalung Tsangpo suture: the upper crust of the research area is a resistive layer with resistivity value range of 200-3 000 ?·m. The depth of its bottom surface is about 15-20 km generally,but the bottom surface of resistive layer is deeper in the middle of these two profiles. At line 900,it is about 30 km deep,and even at line 800,it is about 38 km deep. There is a gradient belt of resistivity at the depth of 15-45 km,and a conductive layer is beneath it with resistivity even less than 5 ?·m. This conductive layer is composed of individual conductive bodies,and at the south of the Yalung Tsangpo suture,the conductive bodies are smaller with thickness about 10 km and lean to the north slightly. However,at the north of the Yalung Tsangpo suture,the conductive bodies are larger with thickness about 30 km and also lean to the north slightly. Relatively,the conductive bodies of line 900 are thinner than those of line 800,and the depth of the bottom surface of line 900 is also shallower. At last,after analyzing the effect factors to the resistivity of rocks,it was concluded that the very conductive layer was caused by partial melt or connective water in rocks. It suggests that the middle and lower crust of the center-southern Tibetan plateau is very thick,hot,flabby,and waxy.  相似文献   

综合物探解决黄土区煤田复杂地质问题     

石君华 《中国煤田地质》2007,19(1):57-59

山西某矿位于构造堆积盆地，属黄土匠陵地貌，区内被第四系黄土覆盖，为解决该矿地质构造及水文地质问题，采用三维地震勘探与瞬变电磁法、直流电测深法相结合的勘探方案。利用三维地震勘探解决目的层赋存形态及其地质构造问题，再利用瞬变电磁法进行平面控制，以使平面及深度解释误差达到勘探要求；应用直流电测深法及瞬变电磁进行勘探，在正反演解释的基础上对其资料综合分析、对比，并结合三维地震资料，确定地质构造的富水及导水性。  相似文献   

直流激电测深二维反演的若干问题研究     

刘海飞  阮百尧  吕玉增 《物探与化探》2007,31(1):47-50,54

目前,激电数据的二维反演主要针对高密度激电数据,而对于常规的激电测深则很少涉及.据此,针对常规激电测深二维反演所涉及到的一些技术难点进行探讨.在正演过程中,根据实测数据实现有限元网格自动剖分,并采用双网格系统,用相邻节点电导率双线性连续进行有限元模拟,并对模拟的误差进行校正.在反演过程中,利用互换原理和Broyden的方法计算偏导数矩阵;采用与奇异值分解算法精度相当的共轭梯度算法求解偏导数矩阵方程.最后通过对模拟数据和实测数据进行反演试算,验证本计算方法是可行的.  相似文献   

贮存环境对气球升空高度的影响初探     

汤文宁 《广西气象》2007,28(1):84-85

施放高度是高空气象探测五项业务考核指标之一，研究气球贮存环境对探测高度的影响，对提高探测高度服有直接的关系。  相似文献   

如何正确使用探空高度代替斜距的方法     

覃晓玲黎洁波  韦丽英 《广西气象》2007,28(1):86-87

对L波段探空系统在使用过程中出现近地层斜距因受地物回波影响而失真的情况，探讨软件所提供代替方法的合理性。  相似文献   

14时探空在改进北京地区对流天气潜势预报中的作用   总被引：4，自引：0，他引：4  

廖晓农  俞小鼎  谭一洲 《气象》2007,33(3):28-32

为了探讨增加14时探空对于对流天气短时临近潜势预报的作用。用1995—2005年北京地区22个人工观测站资料统计了夏季常见的对流天气日变化特征。结果表明，41．6％的雷阵雨、61．3％的冰雹以及58．5％的雷暴大风发生在15—-20时之间。利用探空资料计算并对比了出现在2006年7—9月14时探空释放后到20时期问11个雷暴个例的08时和14时BCAPE、DCAPE、CIN等对流参数。结果表明，对于多数个例，在判断对流是否发生时14时探空优于08时。因此，增加14时探空对于提高对流天气有无预报准确率有帮助。  相似文献   

地面-坑道激电测深方法在山东玲珑断裂带深部找矿中的应用     

李忠平 《地质与勘探》2020,56(4):783-791

在山东玲珑断裂带深部找矿中,考虑断裂带处在地电干扰和地形变化复杂地段,且深部地质体产状变化较大,仅依据半空间地面物探方法很难摸清地质体的展布形态,盲目布设钻孔会造成找矿成本的提高。为精确反演深部矿体的边界范围、走向及倾向,提高钻孔见矿率,降低找矿成本,在山东玲珑断裂带地面、坑道采用立体物探技术,试验通过布设多条方位不同的地-坑、坑-坑和地-地纵横激电中梯剖面和双向三极测深剖面,进行了二维电法剖面反演。在地面-坑道激电测深方法中,地面-坑道供电,坑道测量探测深度与坑道深度呈正相关,反映了深部巷道底板以下电阻率和极化率的分布状况,可以实现深地探测目的。由于地面-坑道供电,坑道测量装置处在半空间和全空间两个部分,需要采用"镜像法"和地下倾斜偶极源电流场特征对其装置系数k值重新推导,以反映坑道空间岩矿体真实电阻率的变化。坑道中梯剖面异常与单向三极剖面异常、双向三极电测深反演结果对应较好。经钻探验证,矿体分布与物探推断高极化体基本一致,为快速准确布设深部钻孔提供资料。  相似文献   

电测深及水文测井在塔里木盆地寻找地下淡水体的研究   总被引：2，自引：0，他引：2  

张建荣 《水文地质工程地质》1998,25(6):54-58

本文通过对多年来积累的水文物探资料的初步分析研究,发现含水层的电性特征与地下水矿化度之间存在着幂函数的变化规律,其相关关系式为Ｍｓ＝３３．９３５３ρｓ＾－１．１４１６和ＭＪ＝３３．５８９２ρｓ＾－１．０４９６,这在近年来寻找地下淡水体方面发挥了重要作用,并取得了良好的社会效益和经济效益。  相似文献   

Optimized and robust experimental design: a non-linear application to EM sounding     

Hansruedi Maurer  & David E. Boerner 《Geophysical Journal International》1998,132(2):458-468

Pragmatic experimental design requires objective consideration of several classes of information including the survey goals, the range of expected Earth responses, acquisition costs, instrumental capabilities, experimental conditions and logistics. In this study we consider the ramifications of maximizing model parameter resolution through non-linear experimental design. Global optimization theory is employed to examine and rank different EM sounding survey designs in terms of model resolution as defined by linearized inverse theory. By studying both theoretically optimal and heuristic experimental survey configurations for various quantities of data, it is shown that design optimization is critical for minimizing model variance estimates, and is particularly important when the inverse problem becomes nearly underdetermined. We introduce the concept of robustness so that survey designs are relatively immune to the presence of potential bias errors in important data. Bias may arise during practical measurement, or from designing a survey using an appropriate model.  相似文献   

Crustal accretion beneath the Koyna coastal region (India) and Late Cretaceous geodynamics     

A.P Singh  D.M Mall   《Tectonophysics》1998,290(3-4):285-297

In 1967 a major earthquake in the Koyna region attracted attention to the hitherto considered stable Indian shield. The region is covered by a thick pile of Deccan lava flows and characterized by several hidden tectonic features and complex geophysical signatures. Although deep seismic sounding studies have provided vital information regarding the crustal structure of the Koyna region, much remains unknown. The two available DSS profiles in the region have been combined along the trend of Bouguer gravity anomalies. Unified 2-D density modelling of the Koyna crust/mantle suggests a ca. 3 km thick and 40 km wide high velocity/high density anomalous layer at the base of the crust along the coastline. The thickness of this anomalous layer decreases gradually towards the east and ahead of the Koyna gravity low the layer ceases to be visible. Based on the seismic and gravity data interpretation in the geodynamical/rheological boundary conditions the anomalous layer is attributed to igneous crustal accretion at the base of the crust. It is suggested that the underplated layer is the imprint of the magmatism caused by the deep mantle plume when the northward migrating Indian plate passed over the Reunion hotspot.  相似文献