河南省吉家洼金矿外围F1含矿带中深部金矿成矿潜力预测

吉家洼金矿是熊耳山金矿田内的一中小型金矿,经建矿开采和探采结合,已持续生产十多年,累计查明金5 379 kg。笔者在系统总结研究以往金矿床的浅表部成矿特征和成矿规律的基础上,认为吉家洼金矿外围F1含矿带的中深部成矿具有半隐伏-隐伏成矿特征。通过少量验证工程的实施和中深部成矿潜力及隐伏矿资源量预测,可获金9 874 kg,表明F1中深部具备找矿潜力,应继续开展中深部找矿的验证工作。这将对该区域深部找矿及寻找隐伏矿具有重要意义。     

湘西江东湾锑金矿床成矿地质特征、控矿因素及深部找矿远景分析

江东湾锑金矿床位于雪峰造山带中段,产在区域主干断裂控制的断块上升隆起区。矿体呈脉状、薄板状赋存于新元古界板溪群五强溪组上段浅变质岩系中。通过矿床成矿地质特征、控矿因素、垂向分带、找矿前景等方面的综合分析,认为江东湾锑金矿床是湘西龙王江金矿集区最具有找矿潜力的矿床。矿床浅部以锑或锑金为主,深部以金为主,且越向深部,金矿化越强,隐伏矿脉增多,深部找矿空间大,具有中型金矿床的资源潜力。     

中国金矿床时空分布规律及地质背景

近年来,中国金矿地质勘查取得了较大的进展,一是大型或具有特大型资源潜力的矿床明显增多,首次发现了单个矿床资源量达到超大型的金矿床(如甘肃阳山、寨上,青海大场等);二是中西部地区或老矿区深部(隐伏)金矿找矿勘查工作取得重要突破(胶东焦家金矿)这些金矿床的     

豫西吉家洼金矿床成矿时代和成矿物质来源:来自闪锌矿Rb-Sr同位素年龄和Pb同位素的证据

豫西吉家洼金矿位于熊耳山金多金属矿集区西部,是一构造蚀变岩-石英脉型金矿床。矿体产于近南北向断裂带中,在倾向上呈"Y"字型分布,矿化以细脉-网脉状、浸染状黄铁矿化蚀变岩型金矿为主,其次为石英脉型金矿。热液成矿过程包括4个矿化阶段,黄铁矿-石英阶段(Ⅰ)、石英-黄铁矿阶段(Ⅱ)、石英-多金属硫化物阶段(Ⅲ)和石英-碳酸盐阶段(Ⅳ)。本次工作对吉家洼金矿床主要成矿阶段(Ⅲ)的闪锌矿进行了Rb-Sr同位素测年研究,以限定成矿时代。结果获得Rb-Sr等时线年龄为118.2±2.4Ma,表明矿床形成于早白垩世。该年龄与熊耳山地区中的庙岭、祁雨沟、公峪等金矿床的成矿年龄基本一致,对于整个熊耳山地区的金矿成矿年龄具有一定的约束意义。锶-铅同位素研究结果显示,吉家洼金矿的成矿物质为壳幔混源,新太古界太华群基底及其重熔形成的花岗岩体可能为铅同位素的主要物源。我们认为,吉家洼金矿床是熊耳山地区在早白垩世区域性强烈的构造-岩浆-流体活动事件的产物,是整个中国东部金的大规模成矿作用的组成部分。     

物化探综合信息找矿方法在萤石矿找矿中的应用

福建光泽地区是闽北地区重要的萤石矿成矿远景区,具有寻找隐伏—半隐伏萤石矿的潜力,但是目前该区隐伏—半隐伏萤石矿找矿成果较少。通过对福建光泽地区I号萤石矿预测区开展物化探综合信息找矿方法应用,探讨物化探综合信息找矿方法在隐伏—半隐伏萤石矿找矿中的应用效果。结果表明:区域水系沉积物测量和大比例尺化探剖面测量圈出的F、Ca等综合异常信息可协助筛选、确定萤石矿找矿目标区;将高精度磁法测量与视电阻率联合剖面测量相结合,可进一步判断萤石矿控矿构造的位置和规模;高密度电阻率法测量可协助确定控矿构造的深部延伸情况。地表检查和深部钻探验证表明:区域化探、高精度磁法测量、视电阻率联合剖面测量和高密度电阻率法测量等物化探综合信息找矿方法组合,可指导隐伏—半隐伏萤石矿的找矿工作。     

西藏扎囊县克鲁铜金矿找矿远景预测研究

在总结克鲁铜金矿产出地质背景、矿床地质特征的基础上,探讨了矿床成因,认为该矿床属中高温接触交代矽卡岩型成因为主。通过对矿区地质、地球化学、地球物理特征的分析与研究,对克鲁铜金矿的深部及其外围找矿远景做出了预测,初步认为克鲁铜金矿的深部及西侧找矿潜力大．是寻找隐伏-半隐伏的矽卡岩型或斑岩型铜金矿的重要远景区。     

广西高龙金矿地电化学深部找矿研究

地电化学提取法是在动态平衡的原理之上，利用人工电场提取深部或成矿离子进行成矿预测，确定成矿靶区。为节省投入和资源，延长矿山寿命，对广西高龙金矿投入以地电化学提取为主的深部找矿方法来找寻延深或下伏矿体。通过对地电化学提取异常和其他物化探异常的综合分析，确定高龙金矿鸡公岩矿段具有一定的找矿潜力，并再次证明了地电化学提取法找寻深部隐伏矿的有效性及其探测深度。     

分形理论在天柱-黎平金矿区深部找矿中的应用

贵州省天柱-黎平地区是我国21个重要成矿区带之-的鄂西-湘西成矿带的南延部分,金矿床(点)分布密集,主要为石英脉型金矿,该类型金矿形态复杂,品位变化大[1],给金矿的预测和探采工程的布置造成了困难[4]。本文利用分形理论以八瓢金矿、官州金矿为例探讨得出了分形理论[2]在天柱-黎平地区深部找矿中有着很好的应用前景,区内深部具有进一步寻找金矿隐伏矿体的潜力,为该区深部找矿提供了一种新思路。     

物化探综合信息找矿方法在萤石矿找矿中的应用

福建光泽地区是闽北地区重要的萤石矿成矿远景区,具有寻找隐伏—半隐伏萤石矿的潜力,但是目前该区隐伏—半隐伏萤石矿找矿成果较少。通过对福建光泽地区I号萤石矿预测区开展物化探综合信息找矿方法应用,探讨物化探综合信息找矿方法在隐伏—半隐伏萤石矿找矿中的应用效果。结果表明: 区域水系沉积物测量和大比例尺化探剖面测量圈出的F、Ca等综合异常信息可协助筛选、确定萤石矿找矿目标区; 将高精度磁法测量与视电阻率联合剖面测量相结合,可进一步判断萤石矿控矿构造的位置和规模; 高密度电阻率法测量可协助确定控矿构造的深部延伸情况。地表检查和深部钻探验证表明: 区域化探、高精度磁法测量、视电阻率联合剖面测量和高密度电阻率法测量等物化探综合信息找矿方法组合,可指导隐伏—半隐伏萤石矿的找矿工作。     

物化探综合信息找矿方法在萤石矿找矿中的应用

福建光泽地区是闽北地区重要的萤石矿成矿远景区,具有寻找隐伏—半隐伏萤石矿的潜力,但是目前该区隐伏—半隐伏萤石矿找矿成果较少。通过对福建光泽地区I号萤石矿预测区开展物化探综合信息找矿方法应用,探讨物化探综合信息找矿方法在隐伏—半隐伏萤石矿找矿中的应用效果。结果表明: 区域水系沉积物测量和大比例尺化探剖面测量圈出的F、Ca等综合异常信息可协助筛选、确定萤石矿找矿目标区; 将高精度磁法测量与视电阻率联合剖面测量相结合,可进一步判断萤石矿控矿构造的位置和规模; 高密度电阻率法测量可协助确定控矿构造的深部延伸情况。地表检查和深部钻探验证表明: 区域化探、高精度磁法测量、视电阻率联合剖面测量和高密度电阻率法测量等物化探综合信息找矿方法组合,可指导隐伏—半隐伏萤石矿的找矿工作。     

Unity of the national and the international in the socio-cultural development of the peoples of the USSR

International unity is becoming ever stronger in this country owing to an increasing similarity in the development of the cultural environment. This comprises the provision of all the country's republics with a sufficient number of schools, theatres, and other institutions and cultural information media in accordance with the needs of the population. An important part is played by the rise in ‘the general educational level, as well as the level of professional qualifications and skills. Among all the Soviet nations and nationalities, this rise being more rapid among formerly backward peoples. Prominent among the factors of internationalization is the progressive development of the nationalities’ cultural resources, while professional culture is being increasingly brought within the reach of the masses.The implementation of the nationalities policy promotes the all-round development of all Soviet nations and nationalities, their drawing together, the upsurge of the individual capabilities of every Soviet citizen.     

Deviation of the major axis of the inertia ellipsoid of the Moon from the direction toward the Earth

It is known from observations that the center of mass of the Moon does not coincide with the geometric center of its figure, and the line connecting these two centers is not aligned with the direction toward the center of the Earth, instead deviating toward the Southeast. This stationary deviation of the axis of the inertia ellipsoid of the Moon to the South of the direction toward the Earth is analyzed. A system of five linear differential equations describing the physical libration of the Moon in latitude is considered, and these equations are derived using a new vector method taking into account perturbations from the Earth and partly from the Sun. The characteristic equation of this system is obtained, and all five oscillation frequencies are found. Special attention is paid to the fifth (zero) frequency, for which the solution of the latitude libration equations are stationary and represents a previously unknown additional motion of the rotational axis of theMoon in a cone with a small opening angle. In contrast to the astronomical precession of the Earth, the rotation of the angular-velocity vector is in the positive direction (counter-clockwise), with the period T ₃ = 27.32 days. On this basis, this phenomenon has been named “quasi-precession.” This quasi-precession leads to a stationary inclination of the major axis of the inertia ellipsoid of theMoon to the South (for an observer on Earth), making it possible to explain one component of the observed deviation of the center of mass of the Moon from the direction toward the Earth. The opening angle of the quasiprecession cone is approximately 0.834″.     

Global repeating events in the history of the Earth and the motion of the Sun in the Galaxy

Chronological analyses of correlations between certain global repeating events (mass extinctions of marine organisms, meteorite impacts, and flashes in the frequency of geomagnetic reversals) during the Phanerozoic Eon and the motion of the solar system in the Galaxy are presented for five rotationally symmetrical models for the regular Galactic gravitational field. Thirteen of sixteen mass-extinction events can be described by a repetition interval of 183±3 million years. This is in agreement with the anomalistic period (interval between two subsequent passages of the Sun through the apocenter of its Galactic orbit) in the model of Allen and Martos. The positions of the minima and maxima in Gaussian functions approximating the frequency distribution for geomagnetic reversals also agree with the times of passage of the Sun through the apocenter and pericenter, respectively, of its Galactic orbit in this model. The maximum in the distribution of the deviations of the dates of mass extinctions from the nearest dates of impacts of large, crater-forming bodies is close to zero, providing evidence that many such events are correlated. As a rule, extinctions follow impact events. The impacts of large bodies have occurred most often when the solar system passes through the Galactic plane, while mass extinctions occur more often at some distance from the Galactic plane (about 40 pc). As a rule, intervals of increases in the frequency of geomagnetic reversals coincide with dates of impacts of large bodies. At the same time, these intervals do not show a clear correlation with the dates of mass extinctions. The intensity of mass extinctions, like the energy released by impacts, is consistently higher in periods when the Sun is moving from the apocenter toward the pericenter of its orbit, than when it is moving from the pericenter toward the apocenter. Thus, there is evidence for a variety of relationships between repeating global events in the Phanerozoic and the motion of the Sun in the Galaxy. Long-period variations in the frequency of geomagnetic reversals are correlated with the orbital motion of the Sun, and increases in the frequency of geomagnetic reversals are correlated with impacts. Mass extinctions are correlated with the impacts of large bodies, whose motions may have been perturbed by clouds of interstellar material concentrated toward the Galactic plane and by the shock front associated with the Perseus spiral arm, through which the solar system passes. The velocity of the Sun relative to the spiral pattern is estimated.     

摩擦桩基桩土间极限摩阻力取值问题探讨

通过对广珠东线高速公路横沥大桥的试桩及土体的工程地质条件分析,总结出影响摩擦桩基桩土间极限摩阻力取值的一般问题以及解决问题的方法和措施。     

从榴辉岩与围岩的关系论苏鲁榴辉岩的形成与折返

位于华北和扬子两板块碰撞带中的苏鲁榴辉岩形成的温压条件不但是超高压，而且是高温。榴辉岩的PTt轨迹表明其为陆-陆磁撞俯冲带的产物。榴辉岩的区域性围岩花岗质片麻岩为新元古代同碰撞期花岗岩，榴辉岩及其他直接围岩皆呈包体存在于其中，并见新元古代花岗岩呈脉状侵入榴辉岩包体中。区域性围岩新元古代花岗岩的锆石中发现有柯石英、绿辉石等包裹体，表明新元古代花岗岩的组成物质也经受过超高压变质作用，且榴辉岩与围岩新元古代花岗岩的锆石U-Pb体系同位素年龄基本相同。但新元古代花岗岩所记录的变质作用和变形作用期次（或阶段）却少于榴辉岩。椐上述可得如下推断：超高压榴辉岩与新元古代花岗岩岩浆是同时在碰撞带底部（俯冲板块前部）形成的；榴辉岩的第一折返阶段是由新元古代花岗岩岩浆携带上升的，其第二折返阶段是和新元古代花岗岩一起由逆冲及区域性隆起而上升，遭受剥蚀。     

某高速公路下伏煤矿采空区稳定性分析

在论述某高速公路下伏砦脖煤矿采空区地质、采矿和工程地质特征的基础上, 进行了稳定性数值模拟分析, 定性与定量地分析与评价了该煤矿采空区的地表变形特征及稳定性。研究结果表明: 该煤矿采空区的变形尚未完成, 对拟建的高速公路将产生很大的危害, 必须采取相应的工程治理措施。      

On the consistency of proposed models for the Pyrenees with the structure of the eastern parts of the belt

The structure of the eastern Pyrenees consists mainly of south-directed thrusts involving basement and cover rocks. An antiformal stack developed by the piling up of basement thrust sheets which outcrop in the Axial zone. These structures account for a thin-skinned thrust model rather than a vertical fault model in which the Axial zone would be essentially autochthonous, and the North-Pyrenean fault the axial plane of a fan thrust system. New data from the Eastern Pyrenees and the thin-skinned model suggest that(1) the structure east of the Pedraforca nappe is similar to that of the Central Pyrenees; (2) the cover rocks of the South-Pyrenean units and of the Axial zone-after restoration—built up a northwards-thickening prism consistent with the existence of a unique Pyrenean sedimentary basin during Mesozoic time; (3) the Axial zone is only a complex antiformal stack developed as a part of South-Pyrenean system related to the Paleogene thrusting-tectonics. The Axial zone palaeogeographic area had no special meaning during Mesozoic time.     

Paleomagnetic implications on the evolution of the tethys belt from the atlantic ocean to the pamirs since the triassic

We first re-examined the apparent polar wander curves for stable Eurasia and Africa since the Triassic. These curves were then combined together with curves of North and South America according to the kinematics of the Atlantic ocean and a synthetic polar wander curve was given. Then, most of the paleomagnetic results from the Tethys mobile belt, from the Atlantic to the Pamirs, were analysed.Several groups of plates, microplates and blocks can be seen. First, relatively stable regions like Maghreb and Sicily, which have not moved much. Then we have a group formed by Iberia, Sardinia, Italy and, to a lesser extent, Corsica and the Western and Central Alps. For these blocks, movements are anticlockwise rotations chiefly driven by the anticlockwise rotation of Africa, but they are sometimes stronger.To the east, a major change takes place. The north of the Aegean Sea and the Ionian zone are clockwise rotated and these rotations are recent: Oligocene-Miocene for the first part, Pliocene to the present for the second part.A major problem arises in Turkey, Caucasus and Iran. Paleomagnetic results indicate a position far to the south of Eurasia, and, at the same time, geological evidence is in favour of a position close to Eurasia. We discuss these discrepancies.