多期走滑拉分盆地的沉积响应:以南海北部珠江口盆地为例

南海北部陆缘位于太平洋和新特提斯两大构造域之间,其形成与演化受到多期多向构造叠加作用,珠江口盆地是南海北部陆缘的重要构造单元.自新生代早期珠琼运动以来,由于太平洋板块向华南大陆俯冲在珠江口盆地形成两期强烈的走滑拉分作用,从而导致早期弥散状地堑与后两期拉分盆地的三层盆地叠合现象.本文在综合珠江口盆地的地质、构造物理和数值...     

关于南海北部特提斯的讨论

南海及邻区处于欧亚大陆与冈瓦纳古陆拼合带的东南端,是特提斯构造域和濒太平洋构造域交汇的重要地区.特提斯缝合带沿金沙江-哀牢山构造带进入南海,人们从而认为南海可能存在特提斯洋遗迹,并认为缝合带存在于磁静区中.本文通过对南海北部陆坡地球物理资料的解释结果,包括重力、磁力、海底地震和深反射地震数据,以及区域地质特征分析,研究了南海北部陆缘高磁异常带和磁静区的成因.结果表明高磁异常带是中白垩世时期古太平洋板块转向俯冲形成的陆缘火山弧,当时存在古俯冲带.磁静区经历了后期大陆边缘张裂和古南海和南海的打开,并经历了高温热物质的底辟作用,使得地壳拉张减薄,居里面抬升形成磁静区.经历了南海的扩张后,原始的俯冲带可能已经向南迁移到南海南部或者已经俯冲消失,其中也不存在缝合带.      

古南海构造属性及其与特提斯和古太平洋构造域的关系

为了进一步理解南海地区前新生代的构造演化过程,明确古南海构造属性及其与特提斯和古太平洋构造域的关系,通过对古南海遗迹（蛇绿岩、蛇绿混杂岩以及俯冲增生带）的研究,结合周围陆区地质及古生物资料,将古南海的演化划分为4个阶段。①古特提斯残留海阶段（T₁-T₂）:古南海是在早-中三叠世的古特提斯残余海基础上发展而来,与古特提斯残余海是一个连续的演化过程。②古太平洋边缘海阶段（T₃）:晚三叠世,由于古特提斯洋的全面关闭,古南海主要受古太平洋的影响。③中特提斯与古太平洋叠加影响阶段（J-K₁）:早侏罗世,古南海开始扩张,并受中特提斯和古太平洋叠加影响;晚侏罗世,南沙地块向华南大陆开始漂移,古南海进一步强烈扩张。④俯冲消亡阶段（K₂末期-E）:晚白垩世,南沙地块开始裂离华南大陆,古南海开始向南俯冲;至始新世,伴随着新南海的扩张,古南海加速消亡于巽他地块之下,并在南海南部地区形成了卢帕尔线蛇绿岩带以及一系列的俯冲增生带。     

太平洋古陆的破碎消亡与中新生代华北克拉通板内构造岩浆活化

回顾了太平洋撞击成因假说的主要内容, 重点围绕太平洋古陆消亡的内外动力学机制进行讨论, 认为P/ T之交发生在太平洋地区的撞击事件撞裂了岩石圈板块, 导致岩石圈下的地幔对流方式发生重大转折.在这种全新的对流方式驱动下, 太平洋古陆板块伴随新生洋壳板块的俯冲和碰撞而逐渐消亡并拼接到环太平洋大陆边缘, 与此同时, 环太平洋构造域开始形成.这种以太平洋构造域为中心的深部构造热体制深刻地影响了环太平洋大陆板块在中新生代的构造岩浆活动.      

南海的形成演化与新特提斯在南海的重新活化

南海位于印度板块、欧亚板块和太平洋板块之间,是世界上最大的边缘海,其构造位置处于太平洋构造域和特提斯构造域,地质构造复杂.关于南海形成演化的动力学机制存在有多种不同观点,其中最重要的一个观点是印度板块与欧亚板块的碰撞致使华南地块和印支地块地幔物质沿东南方向蠕动,从而导致南海的海底扩张.从特提斯的演化规律,以及新特提斯的闭合过程来看,南海并不是特提斯洋的残留海,而是新特提斯在闭合过程中配合印度板块与欧亚板块碰撞导致华南地块和印支地块地幔物质东南方向蠕动的动力学机制下,在南海重新活化的结果.     

试论南中国海盆地新生代板块构造及盆地动力学

南海地处欧亚、印度—澳大利亚和菲律宾海板块的交互带,是西太平洋地区面积最大的边缘海之一,其成因机制和演化过程对探讨特提斯构造域和太平洋构造域相互作用及油气勘探等问题具有重要意义,虽备受关注但仍存争议.综合目前该区及外围已有的大地构造等方面的资料,本文从探讨南海外围的构造格架及中-新生代演化过程入手,分析了南海及外围板块...     

东北亚中生代火山岩研究若干问题的思考

东北亚中生代火山岩包括大陆边缘北北东向线型火山岩带,以及大陆内部俄罗斯西伯利亚、蒙古、中国大兴安岭等面型火山岩带。它们是东北亚古亚洲洋构造域向太平洋构造域转换时期深部地幔地球化学过程以及东亚大陆与古太平洋板块相互作用的产物。对它们的研究涉及古生代古亚洲构造域闭合过程的深部地幔的动力学和地球化学演化历史,以及东亚大陆边缘由被动边缘向活动大陆边缘转换历史。古亚洲域大洋岩石圈向地幔深部潜入而引发的热地幔     

南海及其围区中生代岩相古地理和构造演化

以岩相古地理分析和编图为基础,结合构造变动和岩浆活动资料,阐述了南海及其围区中生代构造演化。中生代时研究区位于欧亚大陆的东南缘,受特提斯域和太平洋域交替复合影响。早三叠世时古特提斯洋经过黑水河盆地东延至南海。从中三叠世开始构造岩相古地理演化出现明显的东西分异。晚三叠世时,受印支运动影响华南地块与印支地块拼合,研究区西部抬升,黑水河水道关闭;而研究区东部和东南部却受古太平洋的影响发生海侵,形成“粤东-西北加里曼丹海盆”,该海盆在早侏罗世遭受更大海侵,导致与中特提斯的良好贯通。中侏罗世在中特提斯发生过短暂海侵而形成“滇缅海”。晚侏罗世至早白垩世是中特提斯洋和古太平洋的俯冲鼎盛期,形成绵延数千km的欧亚大陆东南缘俯冲增生带。文中还讨论了中特提斯向南海延伸的通道、中特提斯与古太平洋对南海中生代演化的交替和复合影响以及南海东北部新近发现的晚中生代俯冲带等问题。     

东北经济区基础地质综合研究业已完成

<正>中国东北地区地处古亚洲洋构造域东端,其前中生代地质历史,主要反映了华北古老地壳的形成、元古宙的大陆裂解和古生代的欧亚大陆形成和陆壳增长的过程,以及古生代褶皱带与中间地块交织的特色.在宏观上,由于受太平洋构造域的叠加和改造,在东亚大陆边缘内带,形成了宏伟的北东走向的火山岩带、     

南海南北共轭边缘伸展模型探讨

通过对南海南北边缘地震剖面的对比,结合周边构造分析,提出南海大陆边缘的裂离经历了两期伸展作用,即早期的简单剪切和晚期的纯剪切伸展作用。简单剪切发生在晚白垩世-早始新世,其动力与太平洋板块俯冲带的后撤、太平洋板块与欧亚板块之间汇聚速率的降低、以及先存北倾缝合带等密切相关。纯剪切发生在中始新世－渐新世－早中新世,剪切作用的转变与古南海的南向俯冲板块拖曳有关。     

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.     

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。      

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。     

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.