Paleo- and Neoproterozoic magmatic and tectonometamorphic evolution of the Isla Cristalina de Rivera (Nico Pérez Terrane, Uruguay)

The Isla Cristalina de Rivera crystalline complex in northeastern Uruguay underwent a multistage magmatic and metamorphic evolution. Based on SHRIMP U–Pb zircon, Th–U–Pb monazite (CHIME-EPMA method) and K–Ar age data from key units several events can be recognized: (1) multistage magmatism at 2,171–2,114?Ma, recorded on zircon of the granulitic orthogneisses and their 2,093–2,077?Ma overgrowths; (2) a distinct amphibolite facies metamorphism at ~1,980?Ma, recorded by monazite; (3) greenschist facies reworking and shearing at ca. 606?Ma (monazite and K–Ar on muscovite) along the Rivera Shear Zone, and finally (4) intrusion of the post-tectonic Sobresaliente and Las Flores granites at around 585?Ma. Lithological similarities, geographic proximity and coeval magmatic and metamorphic events indicate a similar tectonometamorphic evolution for the Isla Cristalina de Rivera, the Valentines Block in Uruguay and the Santa María Chico Granulitic Complex in southern Brazil, since at least 2.1?Ga.     

青海祁漫塔格地区航磁异常特征及找矿前景

利用青海祁漫塔格地区1∶5万高精度航磁资料,结合成矿地质背景、构造特征分析了该区航磁异常特征,并依据知矿(床)点的分布及成矿规律对祁漫塔格地区成矿带进行了划分,筛选了一批重点找矿异常,建立了以航磁异常信息为主的综合找矿标志,进而圈定了多个多金属找矿远景区段.对该区下一步矿产勘查部署提供重要依据,并为地面找矿工作提供重要的找矿线索.     

可控源音频大地电磁法方位非各向同性层状介质Occam反演

目前,可控源音频大地电磁法测深资料反演主要基于各向同性介质,在复杂的地电体中,由于岩石裂隙或矿物形状等原因使得在各个方向的电阻率不同。本文主要探讨更为符合实际地质体情况的方位非各向同性层状介质在正交水平电偶源激发条件下的可控源音频大地电磁数据的反演。运用Occam反演方法,实现了可控源音频大地电磁法方位非各向同性层状介质反演。构建理论地电模型,通过理论模型合成数据的反演算例检验了所实现的可控源音频大地电磁法方位非各向同性层状介质反演算法的有效性和稳定性。同时,不同数据的反演结果表明：方位非各向同性介质的反演应同时使用视电阻率ρsxy、ρsyx和相位?xy、?yx数据。     

大陆岩石圈导电性的研究方法

随着地球科学的进展 ,大陆岩石圈导电性结构的研究越来越引起人们的重视 ,而超宽频带大地电磁测深则是目前用于探测岩石圈导电性最有效的地球物理先进技术。它把现代性能优良的宽频带大地电磁系统 (MT 2 4NS或V5 2 0 0 0 )与长周期智能化大地电磁系统 (LIMS)配套使用 ,采集地面上频率范围为n× 10 -4～n× 10 2 Hz的天然电磁场信号 ,并通过一系列数据处理和反演计算 ,获得深达下地壳和上地幔的地下导电性结构模型。此模型不仅可以提供有关岩石圈地质构造轮廓的信息 ,更重要的是可以间接反映现今地下深部的热结构特征和物质状态分布特点。多年来 ,应用超宽频带大地电磁测深对青藏高原岩石圈导电性结构的研究表明 ,高原的中、下地壳确实是良导电性的 ;它可能说明西藏地壳中普遍存在岩石的局部熔融 ,或地热流体。沿着应县—商河剖面的大地电磁测深研究结果从电性的角度证明了太行山山前断裂为一组向东倾斜的深断裂 ,华北地区岩石圈以其为界划分为东、西两区 ;东区为低阻区 ,与构造活动区的岩石圈导电性特征相符 ;西区为高阻区 ,表现出稳定大陆区岩石圈导电性结构的特点。     

海底MT信号采集电路的设计

设计海底大地电磁信号采集电路，需考虑海底信号特征、海上作业以及海底环境等各种因素。分析表明，除遵循电路设计的一般原则外，海底大地电磁测量要重点解决微弱信号检测、智能化数据采集、海底环境监测和同步记录等4个方面的问题。在设计方案中，电路灵敏度达到微伏级；使用嵌入式计算机实现采集控制；对方位、倾斜、振动、温度等参数进行巡回记录；仪器的时钟精度精准到微秒。所研制的电路经过了室内模拟测试和海洋试验。首次采集到中国海域的大地电磁数据。     

松辽盆地后五家户气田沉积相特征与控气作用

本文对松辽盆地东南部后五家户气田划分出22种沉积微相,建立7种相层序,分析了扇三角洲及三角洲沉积环境对天然气成藏的控制作用。指出了扇三角洲前缘砂体和三角洲前缘砂体较为发育,沉积物源来自气田东北部和东南部两个方向。后五家户气田多为构造—岩性气藏和岩性气藏。     

云南永胜宝坪浅源热液改造型铜矿地质及成因

宝坪铜矿赋存于三叠系下统腊美组中。矿体呈似层状,少量脉状,严格受北北西-北西向构造控制。矿床成因类型属浅源热液改造型铜矿床。     

某滑坡土体土-水特征曲线试验研究

利用能够控制基质吸力的4联式非饱和土直剪仪,对清江流域古树包滑坡滑带土体进行了不同固结应力条件下土-水特征试验,得出了土-水特征曲线并进行了函数拟合。结合土-水特征曲线拟合函数,经过数学推导确定了函数中各个参数的物理意义,建立了能够同时反映固结应力、基质吸力和含水率之间关系的函数表达式,弥补了其他方法不能考虑固结应力的缺陷,对补充和发展土-水特征曲线试验和理论具有重要意义。     

个旧高松矿田大箐东矿段深部铜锡矿床成矿模式

成矿燕山中晚期花岗岩受构造、岩性联合控制,沿断裂“扎根”部位显岩舌、岩枝状产出,形成多层次凹陷,其中的锡铜多金属矿床是个旧矿区最低赋矿标高(900m),也是深部找矿的突破,从而建立深部有利部位四类成矿模式.     

Co‐seismic Faults and Geological Hazards and Incidence of Active Fault of Wenchuan Ms 8.0 Earthquake,Sichuan, China

Abstract: There are two co-seismic faults which developed when the Wenchuan earthquake happened. One occurred along the active fault zone in the central Longmen Mts. and the other in the front of Longmen Mts. The length of which is more than 270 km and about 80 km respectively. The co-seismic fault shows a reverse flexure belt with strike of N45°–60°E in the ground, which caused uplift at its northwest side and subsidence at the southeast. The fault face dips to the northwest with a dip angle ranging from 50° to 60°. The vertical offset of the co-seismic fault ranges 2.5–3.0 m along the Yingxiu-Beichuan co-seismic fault, and 1.5–1.1 m along the Doujiangyan-Hanwang fault. Movement of the co-seismic fault presents obvious segmented features along the active fault zone in central Longmen Mts. For instance, in the section from Yingxiu to Leigu town, thrust without evident slip occurred; while from Beichuan to Qingchuan, thrust and dextral strike-slip take place. Main movement along the front Longmen Mts. shows thrust without slip and segmented features. The area of earthquake intensity more than IX degree and the distribution of secondary geological hazards occurred along the hanging wall of co-seismic faults, and were consistent with the area of aftershock, and its width is less than 40km from co-seismic faults in the hanging wall. The secondary geological hazards, collapses, landslides, debris flows et al., concentrated in the hanging wall of co-seismic fault within 0–20 km from co-seismic fault.