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1.
阿尔泰海西造山带区域变质作用类型与地壳演化   总被引:17,自引:0,他引:17  
新疆阿尔泰海西造山带主要发育两期区域变质作用.第一期变质作用属于区域低温动力变质作用类型,以形成低绿片岩相矿物组合为特征,变质温度较低,而应力作用较强,是造山作用初期热流活动较弱,构造变形强烈环境下的产物.第二期变质作用属于区域动力热流变质作用类型,以形成典型的递增变质带为特征.这一期代表造山作用主期热流活动强烈,伴随有构造变形和岩浆活动.不同的变质作用类型代表了不同的大地构造环境,记录了造山带的演化历史和动力学过程.  相似文献   

2.
新疆阿尔泰阿祖拜地区发育两种类型区域变质作用,第一种为区域低温动力变质作用,第二种为区域动力热流变质作用.阿祖拜地区递增变质带是后者的典型代表之一,从花岗岩体外接触带依次发育矽线石-堇青带、红柱石-十字石带、黑云母-石榴石带,递增变质作用强度呈逐渐减弱趋势.结合变形变质作用特征和同位素年龄,可识别出3个变形变质阶段.早期阶段以区域低温动力变质作用为主,形成绿片岩相变质岩石组合;峰期阶段为区域动力热流变质作用,形成典型的递增变质带;晚期阶段则属退化变质作用.不同变质作用类型代表了不同大地构造环境,记录了造山带演化历史年和动力学过程.  相似文献   

3.
后龙门山变质带的变质时期探讨   总被引:1,自引:0,他引:1  
位于青藏高原东缘之后龙门山变质带的变质作用时期问题,争论日久.笔者通过变质作用、同变质变形作用、岩浆活动等特征分析,结合同位素测年资料,提出后龙门山变质带应属两期区域变质作用之产物.中压相系区域动力热流变质作用属华力西期,区域低温动力变质作用属印支期.  相似文献   

4.
新疆阿尔泰地区冲乎尔递增变质带特征及其演化   总被引:8,自引:0,他引:8  
新疆阿尔泰海西造山带主要发育两期区域变质作用:第一期为区域低温动力变质作用类型,第二期为区域动力热流变质作用类型。冲乎尔递增变质带是后者的典型代表之一,从火山沉积盆地边缘到中心发育十字石-蓝晶石带、黑云母-石榴石带、绿泥石-黑云母带、绢云母-绿泥石带,递增变质作用强度具有逐渐减弱的趋势。结合变质变形关系和变质作用演化特点,将变质作用划分为早期、峰期和晚期3个阶段。早期和峰期为连续的递增变质过程,形成典型的中压型递增变质带,晚期则属于后期的退化变质过程。变质作用演化具有顺时针的p-t轨迹,这种递增变质带的发育特征和变质作用演化特点反映了阿尔泰造山带特定的大地构造环境和地壳演化的动力学机制。  相似文献   

5.
岩石地球化学特征显示,西天山木札尔特岩群成岩于塔里木原始古陆台内部毗邻陆缘活动带部位.后期木札尔特岩群总体经历3期变质作用和4期变形作用改造:早期低角闪岩相区域动力热流变质作用(M1)与前震旦纪塔里木运动(D1)相对应,构成近EW向断续展布的普通角闪石变质相带;主期角闪岩相区域动力热流变质作用(M2)与奥陶纪末至泥盆纪初的俯冲造山(D2)相对应,宏观上构成近NEE向展布的铁铝榴石-矽线石变质相带;晚期中高绿片岩相区域动力退变质作用(M3)与泥盆纪末至石炭纪末期的同碰撞造山(D3)相对应,宏观上构成叠加于先期变质相带之上的具网结状组构的动力变质带.  相似文献   

6.
雪龙山变质带研究新进展   总被引:6,自引:0,他引:6  
雪龙山变质带由古—中元古代工江岩组、中梁子岩组、阿马普岩组及四十驮岩组和白龙里吾巴片麻岩、大宝山片麻岩,以及印支期叠加的箐口塘等两个糜棱岩带所组成。经历了以晋宁期为主,叠加了华力西期、印支期等多期变质,产生了三期结晶面理,主期变质达高绿片岩相→低角闪岩相中压区域动力热流递进变质;受到了同变质期和叠加了喜马拉雅期多期构造变形。原岩为古—中元古代大陆边缘增生复理石建造和钾质花岗岩建造。  相似文献   

7.
Brown  M 李三忠 《世界地质》1994,13(4):19-29
Barrow(1893)提出了三个重要观点:(l)关键性指示矿物的应用可确定变质带并推断区域变质作用的空间特征;(2)递增变质作用的概念;(3)热岩浆平流可能是区域变质作用的一个起因,这些都加深了对变质作用过程的理解。本文通过回顾我们对变质岩石PTt轨迹得出的造山带动态演化的认识,以及考虑到造山带内不同类型区域变质作用的可能起因,来进一步探讨这些论题。通过峰值温度和压力的相对时间关系,对区域变质岩石可区分出两种不同的基本造山带类型。以顺时针PT轨迹为特征的造山带在达到峰值温度前获得峰值压力,变质峰期一般滞后于带内早期变形,高于“正常”传导热流的附加热与超覆量有关。相反,以逆时针PT轨迹为特征的造山带在获得峰值压力前达到峰值温度,变质峰期一般先于带内早期变形或与之同时,高于“正常”传导热流的附加热与深成任人体的就位有关。用于确定PTt轨迹的手段有:变斑晶及反应结构中矿物包裹体序列的应用、温压计、流体包体的应用、诸如Gibbs方法的热力学方法、放射性同位素测年、裂变径迹研究和数字模拟。在合适的岩石中,我们可利用特定矿物共生组合来确定单条PTt轨迹,并且同—造山带内的一套PTt轨迹使我们能够解释变质作用动态演化过  相似文献   

8.
秦岭勉略缝合带两期韧性剪切变形及其动力学意义   总被引:5,自引:0,他引:5  
构造解析表明勉略蛇绿构造混嫖岩带经历了两期韧性逆冲剪切变形,早期剪切变形主要发育于蛇绿岩和火山岩岩片中,与区域变质作用同期,剪切运动方向NW→SE;晚期剪切变形具有NNE→SSW高角度逆冲特点,并使不同岩片推覆叠置,构造缝合带现今主导叠瓦状构造样式。变质变形作用研究显示,两期剪切变形都具有高压-低温性质;综合变形时代以及整个缝合带构造演化,认为它们分别代表了俯冲与碰撞造山期变形,并指示洋壳俯冲和碰撞造山作用均具有斜向特点。  相似文献   

9.
柴北缘锡铁山地区滩间山群构造变形分析   总被引:2,自引:0,他引:2  
初步构造变形分析表明 ,柴北缘锡铁山地区的早古生代变质火山岩系 -滩间山群在加里东期碰撞造山过程中经历了两期构造变形 :第一期为垂直造山带的挤压缩短变形 ,形成一系列紧闭褶皱、区域片理和大型韧性剪切带 ;第二期为平行造山带的挤压缩短变形 ,形成区域透入性共轭破劈理或膝折带。这两期变形是柴北缘加里东期碰撞造山带的斜向碰撞造山过程中不同阶段变形特征的体现。这种构造型式可能对于认识斜向碰撞造山带的构造动力学的转换过程具有重要意义。  相似文献   

10.
在前人研究成果和野外调查基础上,对新资深大断裂变质带特征进行系统总结,从宏观构造、显微构造与组构、岩石矿物学、年代学和地球化学等多学科角度综合研究,分析了新资断裂带各类岩石组构成因,并建立了其活动演化期次。新资深大断裂变质带构造岩主要包括定向组构系列岩石和块状系列岩石,主要是由早期的韧性变形变质作用阶段和晚期的脆性破碎作用阶段先后作用形成。越城岭岩体西侧规模巨大的花岗片麻岩带应属新资深大断裂变质带的一部分,属早期活动的产物,其原岩为越城岭岩体,为断裂变质和动力热流变质作用形成。韧性剪切系列岩石按变形变质强度可分为高温高压韧性剪切带和中温高压韧性剪切带,表明韧性剪切作用具有多期性。新资断裂带活动演化主要经历了四个阶段,始于加里东期,至喜山期均有活动,现在的新资断裂带是经过多个阶段不同类型变质作用由东向西不断迁移和相互叠加的结果。  相似文献   

11.
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.  相似文献   

12.
13.
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″.  相似文献   

14.
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.  相似文献   

15.
16.
摩擦桩基桩土间极限摩阻力取值问题探讨   总被引:1,自引:0,他引:1  
陈银生 《世界地质》1999,18(1):54-59
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。  相似文献   

17.
从榴辉岩与围岩的关系论苏鲁榴辉岩的形成与折返   总被引:4,自引:1,他引:4       下载免费PDF全文
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。  相似文献   

18.
某高速公路下伏煤矿采空区稳定性分析   总被引:10,自引:0,他引:10  
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。   相似文献   

19.
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.  相似文献   

20.
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.  相似文献   

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