黑龙江东部中-新生代盆地演化

黑龙江省东部中-新生代盆地基底由佳木斯地块和完达山地体复合而成.佳木斯地块以加里东期变质岩及花岗岩为主,东缘发育晚古生代和早中生代大陆边缘沉积.完达山地体在中-晚侏罗世就位在佳木斯地块东缘,并在早白垩世早期逆冲到佳木斯地块之上,形成具有前陆盆地性质的大三江盆地.大三江盆地在早白垩世晚期遭受逆冲、走滑构造改造.敦密断裂以北的诸多盆地均属大三江盆地改造后的残余盆地.这些残余盆地和完达山地体之下可能存在隐伏的晚古生代和早中生代大陆边缘沉积.三江盆地东部是古近纪断陷的主要发育区,可能存在一与佳依地堑平行的深断陷.隐伏的大陆边缘沉积和断陷是值得重视的油气勘探领域.     

东海盆地中、新生代盆架结构与构造演化

基于地貌、钻井、岩石测年和地震等资料,分析盆地地层分布、盆架结构、构造单元划分和裂陷迁移规律,结果表明东海盆地由台北坳陷、舟山隆起、浙东坳陷、钓鱼岛隆褶带和冲绳坳陷构成,是以新生代沉积为主、中生代沉积为辅的大型中、新生代叠合含油气盆地;古元古代变质岩系构成了盆地的基底。该盆地不仅是印度-太平洋前后相继的动力体系作用下形成的西太平洋沟-弧-盆构造体系域一部分,而且也是古亚洲洋动力体系作用下形成的古亚洲洋构造域和特提斯洋动力体系作用下形成的特提斯洋构造域一部分,晚侏罗世至早白垩世经历了构造体制转换,盆地格局发生重大变革,早白垩世以前主要受古亚洲-特提斯洋构造体制影响的强烈挤压造山和地壳增厚作用演变为早白垩世以来主要受太平洋构造体制控制的陆缘伸展裂陷和岩石圈减薄作用,经历侏罗纪古亚洲-特提斯构造体制大陆边缘拗陷和白垩纪以来太平洋构造体制弧后裂陷两大演化阶段。白垩纪以来太平洋构造体制的弧后裂陷演化阶段可细分为早白垩世至始新世裂陷期、渐新世至晚中新世拗陷期和中新世末至全新世裂陷期。     

胶莱盆地沉积-沉降史分析与构造演化

基于地表典型露头剖面观察、地震剖面和测井资料解释、沉降史分析,并运用叠合盆地和改造盆地的研究思路,恢复了胶莱盆地白垩纪不同演化阶段的盆地原型及其构造性质。结果表明,该盆地经历了3个显著不同的沉积-沉降阶段。早白垩世莱阳群沉积时期,盆地原型表现为两个NE至NNE向延伸的断陷槽:一个沿苴县—诸城断陷发育,另一个沿牟平—即墨构造带发育,其沉积-沉降中心分别受苏鲁造山带北缘断裂带和牟平—即墨断裂带控制;该阶段沉积-沉降速率发生显著的空间分异,最大沉积-沉降速率在断陷槽,为230～370m/Ma,沿两侧斜坡地带沉积-沉降速率减小,约60m/Ma。早白垩世青山群对应一套中基性至中酸性火山岩,在沂沭裂谷盆地中堆积了一套大盛群河湖相沉积,这个时期是典型的大陆裂谷作用阶段,胶莱盆地演化为火山盆地,盆地沉降速率为35～70m/Ma。晚白垩世盆地原型表现为受东西向断裂控制的不对称箕状断陷,由诸城凹陷、高密凹陷和莱阳凹陷组成,其构造性质属于受西侧郯庐断裂和东侧牟平—即墨断裂控制的右旋拉分盆地;该阶段沉积-沉降速率总体一致,在63～73m/Ma。最后探讨了白垩纪盆地不同伸展阶段的动力学机制。     

中国东北中生代构造体制与区域成矿背景: 来自中生代火山岩组合时空变化的制约

本文系统总结了东北地区中生代火山岩的年代学、岩石组合及其时空分布规律,以便对环太平洋构造体系和蒙古——鄂霍茨克构造体系中生代的演化历史及其东北地区中生代区域成矿背景给出制约。基于火山岩中锆石U——Pb定年结果,东北地区中生代火山作用可划分成六期:晚三叠世(200～228Ma)、早——中侏罗世(173～190Ma)、中——晚侏罗世(158～166Ma)、早白垩世早期(138～145Ma)、早白垩世晚期(106～133Ma)和晚白垩世(88～97Ma)。晚三叠世火山作用主要分布在吉黑东部和小兴安岭——张广才岭地区,前者为A型流纹岩,后者为双峰式火山岩组合,它们共同揭示了古亚洲洋最终闭合后的伸展环境;早——中侏罗世火山岩主要分布在吉黑东部、小兴安岭——张广才岭和额尔古纳地区,吉黑东部和额尔古纳地区早——中侏罗世钙碱性火山岩的存在分别标志着古太平洋板块和蒙古——鄂霍茨克洋板块俯冲作用的发生,而小兴安岭——张广才岭早——中侏罗世火山岩则以双峰式火成岩组合为特征,反映了双向俯冲的弧后伸展环境;中——晚侏罗世和早白垩世早期火山岩主要分布在松辽盆地以西和冀北——辽西地区,前者为碱性——亚碱性的过渡系列,主要由玄武粗安岩、粗安岩和少量粗面岩组成,后者为A型流纹岩或碱性流纹岩组成,这些火山岩形成于加厚陆壳的坍塌或拆沉阶段;早白垩世晚期火山岩广泛分布于东北地区,吉黑东部为钙碱性火山岩组合,而松辽盆地和大兴安岭地区则主要为双峰式火山岩组合,前者标志着古太平洋板块的俯冲,后者与早期加厚陆壳的拆沉和/或类似弧后的伸展环境有关;晚白垩世火山岩主要分布在吉黑东部和陆内,前者为钙碱性火山岩组合,后者为碱性玄武岩,反映了来自东部环太平洋构造体系的俯冲作用。综合上述中生代火山岩的岩石组合及时空分布特征,可以判定:1)环太平洋构造体系对东亚大陆下的俯冲始于早侏罗世,中生代期间存在早侏罗世、早白垩世晚期和晚白垩世三次俯冲事件,其影响的空间范围主要在松辽盆地及其以东地区,陆缘和古俯冲带是寻找斑岩型矿床的有利场所,而陆内的伸展区域主要与浅成低温热液矿床有关;2)蒙古——鄂霍茨克构造体系经历了中生代早期的俯冲事件和中侏罗世及早白垩世早期两次陆内推覆事件,其影响的空间范围主要在松辽盆地以西地区和华北地块北缘,中生代早期的俯冲事件主要与活动陆缘背景下的斑岩型矿床关系密切,而晚侏罗世和早白垩世两次与加厚陆壳拆沉有关的伸展背景有利于多金属矿床的形成。     

中国东南部晚中生代构造作用

濒太平洋西缘,位居东亚陆缘南段的中国东南部,是在EW向古亚洲构造域基底之上发育起来的。研究表明,该区在早、中侏罗世经历了一次从EW向古亚洲构造域向NE向西太平洋构造域的体制转换,其转换位置之一是在南岭一带,其地质标志是侏罗纪盆地内近东西走向的灰色沉积岩层、同位素年龄值为180 Ma左右的双峰式火山岩和中侏罗世A型花岗岩等。到早白垩世,本区已基本完成古亚洲域向西太平洋构造域的体制转换。中国东南部晚中生代火成岩的成因机制基本上可用古太平洋岩石圈消减作用、玄武岩浆底侵作用和地壳深熔作用相结合的模式来解释。日本中央构造线—台湾纵谷带—菲律宾民都洛-巴拉望带是晚中生代古太平洋板块向东亚陆缘的消减带。晚中生代古太平洋板块(伊泽奈琦和库拉板块)低角度(<30°)、快速率(>10cm/a)的俯冲,是西太平洋陆缘区能形成宽阔火山岩带的重要动力学原因。宽阔的火山—侵入杂岩区和6条区域断裂构成了中国东南部晚中生代的基本构造框架。台湾纵谷带为古太平洋板块的俯冲-缝合带,而发育在大陆内部的5条区域断裂则具不同构造属性:长乐—南澳带是晚中生代大陆内部的左旋走滑带,上虞—政和—大埔断裂是古基底隆升区与晚中生代火山—沉积盆地区的分界带,绍兴—江山—东乡—萍乡断裂是晚白垩世—古近纪红     

中国东部及邻区早白垩世裂陷盆地构造演化阶段

早白垩世是中国东部及邻区强烈的伸展裂陷和岩石圈减薄时期。根据裂陷盆地几何形态特征和展布型式 ,将早白垩世裂陷盆地分为泛裂陷型 (燕山—松辽断陷盆地群、蒙古断陷盆地群等 )、狭窄型 (沂沭裂谷系、伊兰—伊通裂谷带 )和菱形状型 (胶莱盆地、三江盆地、鸡西盆地等 ) 3种类型。通过综合分析和对比不同类型裂陷盆地沉积序列和构造演化历史 ,结合郯庐断裂带和秦岭—大别造山带白垩纪构造演化历史的研究成果 ,区分了中国东部早白垩世 2个显著不同的引张裂陷阶段和一个构造挤压反转阶段。早白垩世早期引张裂陷阶段 ( 1 4 0～ 1 2 0Ma)形成了宽广展布的燕山—松辽断陷盆地系和蒙古断陷盆地系 ,沿郯庐断裂带发生右旋走滑活动 ,控制了断裂带西侧南华北伸展走滑盆地和东侧胶莱、三江等和沿敦—密断裂带走滑拉分盆地的发育 ;早白垩世中期引张裂陷阶段 ( 1 2 0～ 1 0 0Ma) ,沿郯庐断裂带中、北段发生裂谷作用 ,形成沂沭裂谷系和伊兰—伊通裂谷带 ;早白垩世晚期 ( 1 0 0～ 90Ma)在区域NW SE向挤压应力场作用下 ,所有早白垩世裂陷盆地发生不同程度的构造反转 ,沿郯庐断裂发生强烈的左旋走滑运动。最后指出 ,太平洋古板块向东亚大陆边缘俯冲诱发的大陆岩石圈底侵作用、拆沉作用、地幔底辟和对流 ,以及来自西部块体     

青藏高原东缘龙门-锦屏造山带的崛起——大型拆离断层和挤出机制

龙门-锦屏山的东缘发育一系列逆冲断裂和飞来峰构造,逆冲作用使山体向东叠置在四川盆地之上。新的野外调查、显微构造分析和糜棱岩石英组构的EBSD测量表明,在龙门-锦屏山的前震旦纪变质杂岩体西缘(即青藏高原东缘)发育一条近NS向的大型韧性拆离断裂,被20Ma以来形成的NW—SE向鲜水河韧性走滑剪切带[1]左行错位80km。青藏高原东缘韧性拆离断裂中黑云母40Ar-39Ar测年获得112～120Ma的年龄,表明龙门-锦屏山的崛起可能与白垩纪开始的垂向挤出机制密切关联。结合四川前陆盆地的沉积及演化特征,认为晚三叠世时期羌塘/东昆仑/扬子陆块的碰撞形成松潘-甘孜造山带,晚三叠世—侏罗纪在其东南缘形成四川前陆盆地沉积;早白垩世龙门-锦屏山开始抬升,晚白垩世快速崛起,在四川前陆盆地沉积之上叠置白垩纪—第四纪再生前陆盆地的沉积。龙门-锦屏山的崛起与白垩纪以来扬子板块岩石圈对于松潘-甘孜地体的陆内俯冲作用有关,使位于中下地壳的变质基底岩石在挤出机制下隆起。     

羌塘盆地东部中生代沉积特征与构造演化

羌塘盆地东部基底由前石炭纪吉塘岩群组成,沉积盖层为晚古生代一白垩纪地层。其中,中生代海相地层在盆地内分布广泛,沉积体系多样,构造古地理转换频繁。中生代盆地包括南羌塘坳陷、唐古拉山隆起带、北羌塘坳陷等3个构造单元,内部又可以划分出不同时期多个次级凹陷和凸起。盆地的发展和演化既受南、北两侧板块结合带控制,又受盆地内部被分划性断裂带围限的各断块差异性活动约束,依次经历了晚三叠世前陆盆地阶段,“北羌塘”早-中侏罗世伸展裂陷盆地发育阶段,多玛侏罗纪-早白垩世早期被动大陆边缘陆表海盆地发展阶段、晚期前陆盆地阶段,晚白垩世南羌塘山间压陷盆地演化阶段。实质上,该盆地是不同时期原型盆地有序叠加而构成的大型叠复式盆地。     

辽西地区中生代盆地构造演化

辽西地区为华北地台北缘阴山－燕山造山带的东延部分，中生代发育火山－碎屑岩沉积盆地。盆地地质分析表明，该区在早白垩世早期之前发育的沉积盆地为挤压型盆地，早白垩世中期以后属伸展断陷盆地。根据沉积－构造分析，该区中生代盆地构造演化可划分为5个构造演化阶段；（1）早三叠世－－早侏罗世；（2）早侏罗世－中侏罗世；（3）中侏罗世－晚侏罗世；（4）早白垩世早期；（5）早白垩世中期－晚白垩世。     

中国东部新生代沉积盆地演化

新生代, 中国东部大陆边缘系统总体受到来自印度、澳大利亚、菲律宾和太平洋板块向欧亚板块下部俯冲碰撞的作用, 在大陆边缘形成一系列边缘海盆地和断陷-坳陷盆地, 主要发育松辽、渤海湾、江汉、苏北、东海、珠江口和北部湾等盆地.基于中国东部沉积盆地的中生代构造背景分析和新生代盆地的分布特征, 对其中的7个主要沉积盆地进行了详细的沉积序列和构造演化分析.通过周缘板块和郯庐断裂的构造演化、火山活动、低温热年代学、气候演变等对比分析, 中国东部沉积盆地的演化可划分为3个阶段: 古新世-始新世、渐新世-早中新世和晚中新世-第四纪.      

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。     

The Importance of the Precipitation and the Susceptibility of the Slopes for the Triggering of Landslides Along the Roads

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.     

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.