辽东半岛五龙金矿床航空电磁场特征及找矿意义     

石连成  骆燕  江民忠  王志宏  朱琳  陈伟  韩鹏辉  陈志鹏 《地质学报》2020,94(10):3106-3119

五龙金矿床位于五龙矿集区中部，是矿集区内规模大的石英脉型金矿。为查明矿集区深部构造及指导深部找矿预测，需结合深部地球物理资料综合分析研究。本文基于五龙矿集区航空探测任务，并结合其成矿地质特征，研究了五龙金矿在平面、剖面、空间等维度的航磁、航空TEM、航空大地电磁特征及其找矿意义。研究表明：平面上矿体位于鸡心沟断裂东侧负磁背景场中NE与近SN、NW向弱磁异常带交汇处，中等 强剩余磁异常带的转折端、梯度带，视电阻率低阻区及中低阻梯度带，深部存在团块状视磁化率高值区；剖面上矿体位于“左低右高，上高下低”的视电阻率梯度带上，呈中低阻、低阻特征及强磁场区至弱磁场区的视磁化率梯度带上，呈浅部“上高下低”、深部“下高上低”的中等 弱磁特征；空间上矿体位于鸡心沟断裂东侧的断裂构造低阻带与岩体高阻异常带的梯度带。五龙金矿地质地球物理找矿标志的建立和深部高视磁化率异常区的存在，表明矿区深部1000~2000m空间与五龙金矿体视电阻率、视磁化率特征相似的地段，仍具有较好找矿潜力。  相似文献   

电性源地-井瞬变电磁法全分量响应特性与探测能力分析   总被引：1，自引：0，他引：1       下载免费PDF全文

陈卫营  韩思旭  薛国强 《地球物理学报》2019,62(5):1969-1980

结合地面电性源瞬变电磁法（TEM）探测深度大和地-井TEM探测精度高的优点，本文提出对电性源地-井TEM进行研究.基于一维正演理论，本文对电性源在地下激发的六个电磁场分量的扩散、分布特性和探测能力进行分析研究.研究结果表明地下瞬变场各分量的分布特征与地面情况类似，但是对地层的探测能力与地面情况存在较大差别.各分量的探测能力与它们的扩散特性有关，其中受积累电荷作用，垂直电场E_z和水平磁场Ḣ_x分量对目标层的反映最为明显，E_x和Ḣ_y分量在地下扩散时受"返回电流"的影响会出现变号现象，使得异常体带来的影响被掩盖，不易被分辨.本文研究结果为发展电性源地-井TEM的施工技术、数据处理与解释，建立了相应的理论基础，获得了对该方法的初步认识.  相似文献   

Rutile inclusions in garnet from a dissolution‐reprecipitation mechanism     

Shyh‐Lung Hwang  Pouyan Shen  Hao‐Tsu Chu  Tzen‐Fu Yui  Yoshiyuki Iizuka  Hans‐Peter Schertl 《Journal of Metamorphic Geology》2019,37(8):1079-1098

Metamorphic garnet commonly contains needle‐like rutile inclusions as well as equant rutile inclusions that surround quartz inclusions and range in size from submicrometer to nanometer. Although the origin of these equant rutile inclusions, that is, exsolution or non‐exsolution, has important implications for petrological and tectonic processes, the crystallographic characteristics of these inclusions have rarely been studied because of the small sizes and analytical difficulties involved. Here, we report the crystallographic characteristics pertinent to the genetic origin of minute equant rutile inclusions in cloudy, nearly spherically shaped garnet domains with Ti‐depleted compositions surrounding quartz inclusions in ultrahigh‐pressure garnet from several diamondiferous Erzgebirge quartzofeldspathic gneissic rock samples. TEM analyses show that the equant rutile crystals in cloudy garnet domains are partially bounded by the low‐energy {100}_rt ± {110}_rt ± {101}_rt facets and have rather random crystallographic orientation relationships (CORs) with the garnet host, with preferential alignment of low‐energy lattice planes, for example, {100}_rt//{112}_grt, for some rutile crystals. Although the rather random CORs are unlikely to be attributed to solid‐state exsolution subjected to the stringent topotactic garnet lattice constraints, the characteristic subhedral {100}_rt ± {110}_rt ± {101}_rt crystal forms of rutile can be rationalized by a metasomatic dissolution‐reprecipitation mechanism via a fluid phase. In this scenario, the quartz+fluid inclusions in garnet were first subjected to decompression microcracking during rock exhumation, followed by dissolution of Ti‐bearing garnet matrix at the crack tips or along the crack surfaces and subsequent reprecipitation of rutile, apatite, gahnite, akdalaite, and Ti‐depleted garnet. The rapid coalescence between rutile and garnet crystals in fluid or direct attachment of rutile crystals onto the dissolving crack surfaces would then yield the rather random CORs as reported here. These results, along with previous work on rutile needles, indicate rather diverse genesis of rutile inclusions in various crystal forms, thus shedding light on the controversial exsolution origin for other inclusion suite/microstructure in minerals.  相似文献   

哀牢山南段长安金矿地质特征及找矿方法研究     

李华  王永华  张星培  艾斯卡尔  周一敏 《地质学报》2015,89(6):1085-1098

长安金矿位于哀牢山成矿带南段,是该成矿带上新近发现的又一大型金矿床。该区为哀牢山地体边缘地壳增生带,主要由深变质岩系组成,区内构造断裂发育,对岩浆活动和成矿作用有显著影响。本文总结了长安金矿的地质特征,并以该区的控矿断裂F6为主要研究目标,以地层岩性电性特征作为约束条件,分别展开了磁法、激电、瞬变电磁和大地电磁等综合物探手段的试验研究。研究结果表明,磁法对于该矿找矿效果不明显,瞬变电磁和大地电磁测深反演的电阻率低阻体,准确界定了控矿断裂F6的位置、倾向、断距以及深部延伸情况,通过激电异常可大致判断矿体的位置。所以在长安金矿区下一步的深部隐伏矿勘查中,结合瞬变电磁、激电、大地电磁等地球物理方法,辅以土壤化探异常进行约束,可以达到快速有效找矿之目的。  相似文献   

大定源瞬变电磁一维自适应正则化反演   总被引：1，自引：0，他引：1  

徐玉聪 《地质与勘探》2015,51(2):360-365

自适应正则化反演对初始模型要求较低,直接对瞬变电磁响应数据进行反演。正则化因子通过计算每次迭代的数据目标函数和模型目标函数自适应的得到,从而快速获得地下的地电结构。本文采用自适应正则化反演算法对大定源回线瞬变电磁一维层状模型进行反演,使用均匀半空间作为初始模型,首次采用模型对深度的二阶导数极小的模型约束,通过典型理论模型的反演计算,证明了TEM自适应正则化一维反演算法拟合效果好、精度高,由于不用反复搜索正则化因子,并且收敛速度快,体现了良好的稳定性和可靠性。  相似文献   

应用瞬变电磁法小线框大电流探测隐伏断层   总被引：1，自引：0，他引：1  

杨农合  王辉  徐小林  吴朝俊  杨宁宁  王宝深 《物探与化探》2011,35(1):80-85

瞬变电磁法小线框、大电流技术在金属矿勘探和地下水的探测中已趋成熟。在长期实践的基础上,分析断层上方出现的感应二次场V2 负值现象和成因,提出断层和次新断层以及地质塌陷的探测方法和数据处理的要点,总结出利用小线框、大电流瞬变电磁法探测隐伏断层的技术方法。钻井验证表明,该方法施工快速轻便,断层点定位准确。  相似文献   

基于MPI瞬变电磁测深一维反演并行算法探究     

柳建新  刘鹏茂  刘颖  童孝忠 《物探化探计算技术》2011,33(5):491-495,462

在瞬变电磁测深反演中运用并行技术可以减少计算时间,提高反演的运算效率。MPI（Message Passing Interface）是目前最重要的并行编程工具,它具有移植性好、功能强大、效率高等多种优点。这里基于在Windows系统下使用FORTRAN和MPICH2相结合的开发工具,编写瞬变电磁并行算法程序,对瞬变电磁一维采用直接反演法,通过理论模型对该算法进行试算,计算结果证明了该算法的正确性、高效性和稳定性。  相似文献   

大回线源瞬变电磁技术在西藏山南地区探矿中的应用     

薛国强 《地质与勘探》2011,47(1):100-106

对大回线源瞬变电磁非中心点场和中心点场响应进行对比讨论,认为核函数具有相似的函数形态和函数性质,因此对于非中心点各分量也可以表示成与中心点垂直分量类似的多项式形式,采用待定系数法,完成视电阻率定义,通过模型检验认为方法可行,结果可靠.使用这一技术时西藏山南地区的帕南、努日等两个矿区进行探测,解释结果与钻探验证一致,取得...  相似文献   

同心补偿式直升机时间域航空电磁法吊舱校准装置研究   总被引：3，自引：2，他引：1       下载免费PDF全文

王世隆  王言章  随阳轶  王琦  林君 《地球物理学报》2011,54(9):2397-2406

直升机间域航空电磁法(Helicopter-borne time-domain electromagnetic method,HTEM)的多次空中仪器校准可消除飞行过程中仪器系统受外界环境的时变影响.吊舱校准装置可解决地面环线方式无法实现的空中飞行过程中仪器校准问题.本文从研究同心补偿吊舱装置模型出发,提出了吊舱装置空...  相似文献   

A new occurrence of retrogressed eclogite from the Sanbagawa belt of southwest Japan and its significance     

Tomoki Taguchi  Shunsuke Endo  Yohei Igami  Akira Miyake 《Island Arc》2019,28(5)

The present paper reports, for the first time, the occurrence of an omphacite‐bearing mafic schist from the Asemi‐gawa region of the Sanbagawa belt (southwest Japan). The mafic schist occurs as thin layers within pelitic schist of the albite–biotite zone. Omphacite in the mafic schist only occurs as inclusions in garnet, and albite is the major Na phase in the matrix, suggesting that the mafic schist represents highly retrogressed eclogite. Garnet grains in the sample show prograde‐type compositional zoning with no textural or compositional break, and contain mineral inclusions of omphacite, quartz, glaucophane, barroisite/hornblende, epidote and titanite. In addition to the petrographic observations, Raman spectroscopy and focused ion beam system–transmission electron microscope analyses were used for identification of omphacite in the sample. The omphacite in the sample shows a strong Raman peak at 678 cm^?1, and concomitant Raman peaks are all consistent with those of the reference omphacite Raman spectrum. The selected area electron diffraction pattern of the omphacite is compatible with the common P2/n omphacite structure. Quartz inclusions in the mafic schist preserve high residual pressure values of Δω₁ > 8.5 cm^?1, corresponding to the eclogite facies conditions. The combination of Raman geothermobarometries and garnet–clinopyroxene geothermometry gives peak pressure–temperature (P–T) conditions of 1.7–2.0 GPa and 440–540 °C for the mafic schist. The peak P–T values are comparable to those of the schistose eclogitic rocks in other Sanbagawa eclogite units of Shikoku. These findings along with previous age constraints suggest that most of the Sanbagawa schistose eclogites and associated metasedimentary rocks share similar simple P–T histories along the Late Cretaceous subduction zone.  相似文献