南美奥连特前陆盆地斜坡带低幅度构造形成物理模拟

奥连特盆地是一个位于南美安第斯山前的弧后前陆盆地,盆地东部斜坡带发育大量低幅度构造,并与油气有密切关系。为明确奥连特盆地东部斜坡带低幅度构造的形成过程及其主控因素,深入分析了低幅度构造的发育特征,针对性地开展了构造物理模拟实验研究。结果表明,奥连特盆地东部斜坡带低幅度构造主要与逆断层、反转断层和走滑断层相伴生,一般位于断层上盘,控制其发育的动力学机制主要是断层的正反转作用和走滑作用,而且先存正断层向深部变缓,有利于断层后期的反转以及低幅度构造的发育。     

松辽盆地南缘十屋断陷构造物理模拟研究

松辽盆地十屋断陷早期伸展阶段形成断陷和坳陷沉积,晚期挤压阶段发生盆地反转。采用铲形和直线形2种边界断层模拟十屋断陷的形成和演化过程。模拟实验结果表明,较陡的主干断层控制的半地堑断陷在侧向挤压过程中发生盆地反转,但是早期形成的正断层不一定发育成为反转断层,而是正断层的倾角变陡,并导致在断陷内的上部盖层中发育形成新的逆断层。这一实验结果较好地解释了松辽盆地十屋断陷的构造演化特征,即断陷期形成的正断层在后期反转构造中受到挤压时发生产状变化并在拗陷期沉积盖层中发育逆断层     

先存断层产状及其组合关系对反转构造变形影响的离散元数值模拟研究

反转构造在我国含油气盆地中广泛发育,对于油气勘探具有重要意义.本文采用离散元颗粒流方法研究了先存正断层的陡缓程度、倾向组合关系和距离挤压端的远近等因素对断层的反转构造发育及其反转量的影响.模拟结果显示,先存断层的产状及其距离挤压端的远近会影响先存断层的反转次序、反转量,进而影响盖层内反转构造的发育.当先存正断层倾向指向...     

孙吴—嘉荫盆地沾河断陷构造变形及其对沉积作用的制约

为了揭示孙吴—嘉荫盆地的构造特征、构造变形及其对沉积作用的制约,本文对沾河断陷的地震剖面进行了精细地质解释和相应的研究工作。沾河断陷为孙吴—嘉荫盆地的一个一级构造单元,自白垩纪开始主要经历了2个构造变形阶段：下白垩统宁远村组—淘淇河组上段下部沉积时期为NW—SE向伸展作用阶段,形成NE向大型犁式正断层及由其控制的箕状断陷,盆地连续接受沉积,断陷的沉降中心始终位于控陷正断层上盘靠近断层的部位,断陷盆地的规模与沉积范围随着控陷断层规模和断距的增大逐渐扩展,盆地具有裂谷盆地的性质;下白垩统淘淇河组上段上部—新近系孙吴组沉积时期为NW—SE向挤压作用阶段,形成反转构造、断层传播褶皱和走滑构造。在反转作用过程中,早期伸展断陷受到强烈改造,不仅在断层上盘靠近断层的部位形成大型反转背斜,而且使远离控陷断层的断陷缓坡带发生旋转式隆升,盆地的沉降中心迁移到盆地中间部位;随着反转背斜的隆升速率逐渐大于断陷缓坡带的隆升速率,盆地的沉降中心也逐渐向盆地的NW侧迁移,盆地绝大部分区域的沉降速率、沉积速率始终大于隆升速率,地层是连续沉积的,不存在沉积间断。仅在永安村组—鱼亮子组沉积时期,反转背斜带较高部位的隆升速...     

海拉尔盆地乌尔逊凹陷构造变形对沉降中心迁移的控制

海拉尔盆地是叠置于内蒙-大兴安岭古生代碰撞造山带之上的中、新生代盆地,乌尔逊凹陷是海拉尔盆地中部的1个二级构造单元,自早白垩世开始,经历了3次伸展作用、2次挤压作用,盆地中地层厚度和沉降中心的迁移主要受同生断层和与之伴生的断层相关褶皱所控制。在伸展作用时期：当发育1个犁式正断层,在其上盘形成1个箕状断陷,沉降中心位于断层上盘、靠近断层的区域,在伸展量较大的部位形成1个或多个沉降中心;当发育多个控陷正断层,在其上盘形成多个相互独立的箕状断陷,但每一个断陷都有各自的沉降中心,不同方向断层的交汇部位往往就是断陷的沉降中心。随着伸展量的增大,断陷的沉降中心不断向控陷正断层滑动的相反方向迁移,盆地的规模也随之增大。在第一次挤压作用中,早期NS向控陷断层F₁发生反转作用,其上盘靠近断层的部位发生隆升,远离断层的部位作为大型断层传播褶皱背斜前翼也发生旋转式隆升,乌尔逊凹陷成为NS向大型断层传播褶皱背斜的前翼向斜,地层的沉积厚度在靠近断层的部位和远离断层的部位都很薄;向大型断层传播褶皱背斜前翼向斜部位,地层的沉积厚度逐渐增大,盆地的沉降中心向向斜的低洼区域迁移。在第二次挤压作用中,早期NS向控陷断层F₂发生反转作用,在乌尔逊凹陷中部形成1个规模较大的NS向断层传播褶皱背斜或突发构造,背斜或突发构造的顶部被剥蚀,盆地的沉降中心位于中部背斜带前、后翼向斜的低洼区域。     

从反转构造的砂箱模型看柴达木早-中侏罗世盆地的构造性质

设计了基底均匀伸展半地堑正反转、基底均匀伸展书斜式正反转和对称地堑正反转等3个砂箱实验模型,着重研究后期构造反转对前期正断层构造的叠加与改造作用.单侧挤压实验结果表明,正反转过程中,挤压变形主要通过形成新的低角度逆冲断层实现,前期正断层多数可被保存下来,仅倾角不同程度地变陡.前期正断层全部反转为逆断层的可能性极小,仅在强烈逆冲变形带,逆冲断层才有可能完全取代前期的正断层.根据实验结果并结合柴达木盆地的实际资料,认为柴达木盆地早-中侏罗世时期为挤压性质的盆地.     

乍得Bongor盆地反转构造特征及形成机制：来自地震剖面及沙箱模拟实验的证据

结合区域地震剖面解析和沙箱模拟实验,探讨分析了乍得Bongor盆地反转构造特征及其形成机制。结果表明：（1） Bongor盆地中发育三种典型的反转构造类型：挤压反转单斜构造、挤压反转向斜构造和挤压反转背斜构造。该类反转构造 一部分具有反转断层相关褶皱样式,主要沿高角度边界断层和基底地垒边界断面发育,形成演化与断裂活动息息相关,另 一部分呈散花状背斜构造样式,属于地层纵弯上拱褶皱,主要发育于斜坡断阶带之间;（2） 区域剥蚀作用对盆地反转构造 演化具有重要的影响,其对盆地内深部地层反转褶皱发育具有促进作用,为深部构造圈闭形成提供条件,而对浅部地层的 反转褶皱发育则表现出阻碍或破坏作用,不利于浅层构造圈闭的形成。     

海拉尔盆地红旗凹陷早白垩世构造特征与变形期次的厘定

海拉尔盆地是叠置于内蒙-大兴安岭古生代碰撞造山带之上的中-新生代盆地,总体上呈北东向展布,由三坳、两隆5个一级构造单元组成,自西向东依次为扎贲诺尔坳陷、嵯岗隆起、贝尔湖坳陷、巴彦山隆起和呼和湖坳陷, 其中红旗凹陷是位于贝尔湖坳陷北部的一个二级构造单元。研究表明,红旗凹陷在早白垩世经历了4个变形阶段：在早白垩世兴安岭群-南屯组沉积时期为NW-SE向伸展作用阶段,形成以大型犁式正断层为控陷断层的NE向箕状半地堑;在大磨拐河组-伊敏组一段沉积时期为NW-SE向挤压作用阶段,使早期控陷正断层发生强烈的反转作用而转化为逆断层,靠近控陷断层的NW边界由于断层上盘的逆冲而隆升,凹陷的SE斜坡带由于控陷断层在反转作用过程中深部的逆冲滑移在浅部受阻而发生的旋转式隆升,使凹陷的规模发生明显萎缩,并在凹陷的中部形成大型NE向断层转折褶皱,构成了红旗凹陷的中部断隆带;在伊敏组二段下部沉积时期为近EW向伸展作用阶段,早期控陷断层表现出正断层的特征,新形成的NE向控陷断层具有左行离散型走滑的性质;在伊敏组二段上部沉积时期为近EW向挤压作用阶段,早期控陷断层再次表现为上盘逆冲的特征,在断层上盘、靠近断层的部位形成反转背斜,并在凹陷中形成断层转折褶皱。在每一变形阶段中,红旗凹陷的构造特征在空间上存在一定的差异。     

塔西南坳陷甫沙构造带正反转构造及其石油地质意义

塔西南坳陷甫沙构造带褶皱冲断强烈,古近系膏泥岩下层构造变形复杂,具有正反转构造变形特征。侏罗纪—白垩纪区域伸展环境发育大量正断层,后期在喜马拉雅运动中受挤压反转。南部发育高角度基底卷入正反转断层,中部发育叠瓦式逆冲断层,北部边缘变形微弱。相应地将甫沙构造带划分为反转断隆背斜带、楔状叠瓦构造带和逆冲前缘构造带;反转程度南强北弱、西强东弱。对区域构造变形环境的分析表明,西昆仑山隆升引发水平挤压叠加垂直向上的剪切作用,使先存高角度正断层容易被迁就利用进而发生正反转。对正反转相关构造圈闭评价认为:反转断隆背斜带发育的圈闭规模大,幅度低,埋藏浅,落实程度高,但上覆膏泥岩层薄,被断层破坏强烈,油气散失严重;楔状叠瓦构造带发育的圈闭规模小,幅度大,埋藏深,落实程度低,上覆膏泥岩层厚,有利于油气保存;逆冲前缘构造带发育低幅度隆起和地层岩性圈闭。     

松辽盆地北部白垩纪末反转变形的三维构造物理模拟

构造物理模拟对构造反转机制分析和地震资料的构造解释和模型建立至关重要.作者在深入研究松辽盆地的基底、形成发育和改造史的基础上,对松辽盆地进行6次能再现可重复性的三维构造物理模拟,探讨了断陷盆地晚期反转变形的动态过程,表明在同一构造应力场作用下因受基底中构造边界的制约而可能产生多组方向的背斜构造带.先存的边界条件还决定了晚期变形的产状：断面缓的一侧率先变形,对应的背斜带翼部陡且褶皱幅度大;它还制约了呈雁列式展布的正断层的发育.松辽盆地不同方向的正向二级背斜构造带均为明水组沉积后（白垩纪末）同一挤压应力场作用的结果,该期反转变形控制了新生代松辽地区的沉积发育.     

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.