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1.
华北板块与扬子板块于加里东晚期沿商丹带发生碰撞的同时,在扬子板块北缘,即现今南秦岭构造带,开始发育一条近东西向延伸的拉伸带,其中包括武当地块伸展滑脱构造、武当地块古生代大规模基性岩浆活动及其西侧紫阳-岚皋古生代碱性岩浆活动带、镇安-旬阳浅层塌陷盆地以及佛坪隆起等.该伸展构造带主体在时间上发生在秦岭两期碰撞事件之间,空间上位于南北两个缝合带之间,因此,是秦岭造山带演化过程中的一个非常重要的阶段.该伸展构造的开始很可能与南、北秦岭碰撞后的造山带重力塌陷有关,随着该伸展带南侧晚古生代勉略洋的形成,南秦岭逐渐演化为华北板块南侧的被动大陆边缘,从而使南秦岭的地壳伸展一直延续到早一中三叠世.武当地块伸展滑脱系统中顺层侵位的基性岩席群的年代学与岩石地球化学的研究表明,这些基性岩与勉略蛇绿岩组合中的变辉绿岩及变基性火山岩具有很大的相似性,因此勉略洋很可能也是南秦岭这次拉伸作用的结果.  相似文献   

2.
武当地块主要地质事件年代学研究   总被引:2,自引:0,他引:2  
武当地块是南秦岭构造带内一系列前寒武纪地块之一 ,古生代以来经历过 3次重要的构造变形 ,即伸展作用、逆冲推覆作用和造山晚期走滑构造作用。运用4 0 Ar/39Ar阶段升温、4 0 Ar/39Ar激光探针及Sm Nd等时线等多种测年方法确定伸展构造发生于 4 2 3~ 2 6 1Ma、逆冲推覆构造发生于 2 34~ 2 0 0Ma ,表明伸展构造可能分别与商丹缝合带的碰撞及勉略洋的拉开有关 ,称之为同碰撞伸展构造 ,而武当地块内发育的逆冲推覆构造则应是华北板块与扬子板块沿勉略带发生碰撞的结果。  相似文献   

3.
武当地块基性岩度群岩石地球化学特征及其大地构造意义   总被引:6,自引:0,他引:6  
南秦岭构造带武当地块核部的基性岩席群,是在古生代地幔底侵作用导致地壳伸展过程中岩浆沿主拆离面及基底变质岩群内次一级滑脱面侵位形成。岩席群岩石地球化学特征的研究表明,其主元素、微量元素及稀土元素地球化学与勉略缝合带发育的蛇绿岩组合中的辉绿岩和大洋玄武岩之岩石地球化学特点相似,结合同位素地质学资料,本认为武当地块基性岩席群所代表的这次拉伸作用与略洋的打开是同一构造背景下不同阶段的产物。  相似文献   

4.
秦岭造山带武当地区古生代伸展构造   总被引:15,自引:1,他引:14       下载免费PDF全文
武当地块位于勉(县)略(阳)地区东侧,南部逆冲于扬子板块北缘之上,中-晚古生代期间曾经历过一期伸展构造作用。伸展构造系统以现今中元古代武当山群与新元古代耀岭河组之间的界面为主滑脱面,盖层系统由南往北滑脱拆离。沿主滑脱面上、下侵位了大量的基性岩席,其单颗粒锆石U-Pb年龄为401±14Ma和407±12Ma。滑脱系统上部次级滑脱面上新生白云母的40Ar-39Ar年龄为282±8.5Ma和261±0.25Ma,表明伸展作用可能一直持续到二叠纪。考虑到邻区同时代的碱性岩浆作用,作者认为伸展构造是伴随着古生代大规模的上地幔基性岩浆的底侵作用发生的,很可能代表了勉略洋打开的早期阶段。这对认识秦岭造山带的构造演化具有重要的意义。  相似文献   

5.
秦岭造山带板缘裂解与拼合过程及动力学分析   总被引:1,自引:0,他引:1  
秦岭造山带与原特提斯洋、占特提斯洋扩张作用同步,于震旦世至早奥陶世阿伦尼克期、泥盆纪至早三叠世分别以商丹洋和勉略洋(海)为中心发生两次洋、陆扩张运动,实现了华北板块与扬子板块之间以及各自板缘带的全面裂解破碎,从而形成复杂而不规则的板缘构造带。在主造山期继商丹古洋盆和勉略古洋(海)盆扩张之后分别于早奥陶世、早三叠世晚期开始转变为俯冲消减,并先后于晚古生代末期和中、晚二叠世实现拼合造由,由于商丹古洋壳俯冲消减受到勉略古洋盆同时期的扩张作用影响,秦岭造山带之中的华北板块与扬子板块碰撞过程首先表现为板缘区南方的微地块(或微板块)与北方华北板  相似文献   

6.
武当地块主要地质事件年代学研究   总被引:12,自引:0,他引:12  
武当地块是南秦岭构造带内一系列前寒武纪地块之一,古生代以来经历过3次重要的构造变形,即伸展作用逆冲推覆作用和造山晚期走滑构造作用。运用^40Ar/Ar阶段升温、^40Ar/Ar激光探针及Sm-Nd等时线等多种测年方法确定构造发生于423~261Ma、逆冲推覆构造发生于234~200Ma,表明伸展构造可能分 与商丹缝合带的碰撞及勉略洋的拉开有关,称之为同碰撞伸展构造,而武当地块内发育的逆冲推覆构造则  相似文献   

7.
南秦岭造山带武当地区构造变形及构造复合   总被引:1,自引:0,他引:1  
位于扬子地台北缘的武当推覆体是南秦岭造山带的重要组成部分,它经历了温长的构造演化历程。该区的层圈性结构和加里东-晋宁期的伸展滑脱作用造成了武当群构造堆垛岩系的形成,华北板块和扬子板块在印支运动期间的会聚碰撞造作用使武当巨型推体逐形成,至喜山运动时期完全定位。  相似文献   

8.
丹凤—信阳蛇绿混杂带作为秦岭—大别碰撞造山带主缝合带,其南部属于扬子板块北部大陆边缘。研究区域位于东秦岭南翼,是扬子板块北部大陆边缘的一部分。①晚元古—中震旦世,扬子板块北缘(东秦岭段)为活动型大陆边缘,发育有陡岭岛弧和武当弧后盆地;②晚震旦—早古生代,扬子板块北缘转为被动型大陆边缘,陡岭古岛弧构成边缘地块,武当古弧后盆地演化为边缘盆地;③早古生代晚期,华北板块南缘的秦岭岛弧首先与扬子板块北缘的陡岭边缘地块(古岛弧)碰撞,造成武当边缘(古弧后)盆地的闭合,并形成刘岭前渊和二峪沟前陆盆地;④由于岛弧—边缘地块碰撞加之弧后和边缘盆地的存在,因此在早古生代末期,秦岭—大别山并未大规模隆起,造山带只具雏形。直至中生代早期,华北与扬子两个板块间进一步的陆内俯冲作用才使秦岭—大别山大规模隆起。陡岭古岛弧和武当古弧后盆地的确认合理地解释了秦岭—大别碰撞造山带“加里东碰撞不造山,印支造山不碰撞”的“矛盾”现象。  相似文献   

9.
杜远生  盛吉虎 《地质论评》1999,45(6):563-570
南秦岭西段勉略构造混杂岩带是由不同的构造岩片组成的非史密斯地层区。本文建立了勉略构造带太古宙-石炭纪的地层系统。勉略构造带及其邻区地层格架分析表明晚震旦世--寒武纪勉略构造带及中秦岭为扬子板块北缘的一部分。奥陶纪--志留纪大致沿勉略构造带秦岭型陷槽。泥盆纪-石炭纪该裂陷槽进一步开裂形成勉略洋。该洋盆从石炭纪开始俯冲萎缩并最缍三叠纪后期碰撞、闭合并造山。  相似文献   

10.
南秦岭勉略构造混杂岩带非史密斯地层系统和地层格架   总被引:2,自引:0,他引:2  
南秦岭西段勉略构造混杂岩带是由不同的构造岩片组成的非史密斯地层区。本文建立了勉略构造带太古宙—石炭纪的地层系统。勉略构造带及其邻区地层格架分析表明晚震旦世—寒武纪勉略构造带及中秦岭为扬子板块北缘的一部分。奥陶纪—志留纪大致沿勉略构造带形成南秦岭裂陷槽。泥盆纪—石炭纪该裂陷槽进一步开裂形成勉略洋。该洋盆从石炭纪开始俯冲萎缩并最终于三叠纪后期碰撞、闭合并造山。  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.
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   

13.
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.
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   

16.
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   

17.
18.
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   

19.
In order to characterise the influence of the heavyrains on the observed landslides during the 1996–1997hydrological cycle, rainfall records for the last 100years are analysed from 104 stations in easternAndalusia. Regarding the amounts of rain recordedbetween October 1996 and March 1997 in the 104stations studied, 31 presented new all-time records;15 presented values that were 80–100% of thepre-1995 record; 49 stations, 80–50%; and 9stations, < 50%. A map has been devised of thesusceptibility of the materials through which thesouth-eastern Andalusian road network crosses,together with an inventory of the damage caused byinstability phenomena on banks and cuttings of theroad network during the winter of 1996–1997. Therelationships between the rainfall during the studyperiod, the damage caused to the road network and thesusceptibility of the materials affected are analysed.The results indicate that there is a clearcorrespondence between the rainfall recorded and thesusceptibility of the materials with the inventorieddamage. It is concluded that the widespread seriousdamage caused in early 1997 to the roads andsurrounding areas in the Alpujarra region and thecoast of the Province of Granada was mainly caused bythe extraordinarily heavy rains. However, considerablyless damage was observed where the susceptibility ofthe terrain is low, thus highlighting the extremeusefulness of terrain-susceptibility maps for riskprevention and territorial planning.  相似文献   

20.
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   

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