挤压型盆地构造热演化模拟研究综述

挤压过程对地质构造和沉积盆地的形成演化具有重要的作用.研究挤压型盆地的构造热演化模拟对认识岩石圈内部应力分布、力学属性和流变结构具有重要意义.本文介绍了挤压型盆地构造模拟的弹性模型、粘弹性模型和深度控制的弹塑性模型,对比了这几种模型的优缺点和适用范围.简单介绍了前人在研究地壳隆升时用到的几种热演化模拟方法.虽然挤压过程的构造模拟已经取得了很大进展,挤压型盆地的热演化模拟则具有很大的发展空间,这应是进一步研究的重点.     

太平洋盆地勒夫波与瑞利波不一致性的研究

在勒夫波及瑞利波频散反演的基础上,本文分析了太平洋盆地水平剪切波速度SH与垂直剪切波速度SV之间的不一致性,并对其成因及与地球各向异性之间的关系进行了探讨。我们发现:除最顶部一二十公里处的SH小于SV之外,在几乎整个太平洋岩石圈内,SH都大于SV。此外,在占太平洋大约2/3的区域下面的软流圈内,SH略高于SV。如此广泛存在的SH与SV的不一致性可能是与大规模地质及构造过程有关的太平洋地壳及上地幔的固有各向异性的一个证据。     

陕西省数字地震台下方壳幔速度结构研究

利用广义反、透射系数的传递矩阵计算理论地震图，用快速模拟退火法搜索最佳模型，通过与地震台站实际记录的P波波形进行拟合对比，反演了陕西省13个数字地震台下方的P波速度结构。台站分布区域涉及到秦岭造山带、渭河盆地及鄂尔多斯地台三个构造区域。结果显示，3个构造区的地下速度结构差异明显，呈现了各自的构造特点。其中秦岭造山带上地壳乃至地表速度高，中下地壳出现多个低速层，可能与岩石脱水、构造滑脱带等有关；渭河盆地内上中地壳高低速度层交替出现，反映了断层活动在浅部的影响；鄂尔多斯地台有部分台站保持稳定的匀速构造。反映了古老地台地层稳定发展的特性，部分台站受到后期改造，低速层位增多。因为变化剧烈的台站分布在盆地的南部和西部。而且震源机制解显示该区主应力场方向为近东西向，可以说秦岭北缘的断裂作用以及后来来自青藏高原的挤压应力是导致渭河盆地形成和发展的主要因素。最后我们讨论了速度结构与强震、地震分布以及不同构造演化的关系。     

不对称盆地形成机制探讨：以渭河盆地为例

本文首先讨论了渭河盆地的不对称性,并提出了不对称盆地主控断裂和次控断裂的概念。渭河盆地的不对称性主要表现在:(1)盆地的横剖面形态不对称;(2)盆地南北两侧边界断裂的构造特征及其活动性具有明显的差异性;(3)深部构造形态不对称。最后,以渭河盆地为例,建立了“悬臂梁模型”,对不对称盆地边界控制断裂的发展演化以及形成机制进行了计算分析和讨论。计算结果表明:(1)弯曲导致应力集中,并形成拉破裂;(2)破裂陡倾向自由端;(3)当梁的长度增大时,有可能在固定端形成新的拉破裂。     

板内盆地地震构造分析──以江苏南部为例

板内地震构造的主要控制因素是区域构造应力场和局部的特殊发震构造条件。本文提出江苏南部强地震的主要构造标志是新生代活动盆地，盆地内的隐伏发震断层与区域构造应力场的最大主应力之间的夹角正好有利于剪切破裂的发生。三维有限元数值模拟证明，盆地形成过程中产生的地壳脆弱化，导致构造应力的重新分布和局部集中，盆地内部脆弱体中的隐伏断层是潜在的震源破裂面，盆地边缘积累的弹性应变能则是地震时释放的能量来源。     

辽河盆地新生代多期构造热演化模拟

针对辽河盆地新生代拉张多期性的特点,提出一种适用于多期拉张盆地构造热演化模拟的纯剪切模型．该模型考虑了多期拉张的继承性、横向不均匀性以及拉张速率的可变性。通过几种拉张速率模式的对比,指出拉张速率模式的选择对模拟年轻盆地热演化过程具有重要意义．最后,利用该模型模拟研究了辽河盆地新生代的构造热演化历史．     

复杂场地对地震波传播的影响

本文基于两相介质动力学方程组，利用显式集中质量有限元结合透射人工边界，研究了复杂介质情况下盆地和凸起地形对地震波传播的影响。研究表明，控制波在盆地传播的主要因素有沉积层和基岩的剪切波速比、沉积层的厚度、饱和度。欠饱和土的基本共振频率小于单相土和饱和土的基本共振频率。凸起地形对地震动有放大作用，但是在山脚附近有抑制作用。饱水土的地形效应要比单相土的地形效应更加明显。山间峡谷的放大作用和两山间的距离有密切的关系。     

基于盆地效应的抗震设防研究之若干进展

沉积盆地能够加重震害,在抗震设防中需要定量考虑盆地效应。本文叙述了盆地效应的主要表现形式以及对震害的影响;详细介绍了盆地效应的研究方法以及取得的研究成果,同时也指出了各个方法的优缺点;讨论了抗震设防中对盆地效应考虑的必要性;着重回顾和总结了当前在抗震设防中考虑盆地效应的两种方法:（1）在场地地震动预测模型中加入盆地基底埋深项。（2）求取盆地模型相对一维层状模型的附加放大因子,提出针对当前抗震设防规范中地震动参数的校正系数。最后指出开展盆地抗震设防研究面临的问题及工作展望。     

山西断陷带地壳结构的接收函数研究

利用2006年8月到2008年3月北京大学在山西断陷带南部架设的两条东西向流动观测地震台阵记录的远震资料,提取各台站接收函数,然后进行倾斜叠加(Slant stack)和台阵偏移成像,获得了沿台阵横穿山西断陷带的地壳和上地幔的精细结构变化.研究结果显示,山西断陷带下面莫霍面存在明显不连续,莫霍面上隆约4~6 km,纵横波速比从两侧的1.75上升为山西断陷带内部2.0左右,且中、下地壳可能存在一个低速层.山西断陷带的构造模式沿相距140 km的两条剖面表现出明显差异:南端的临汾盆地为拉张作用下的纯剪切模式,向北转化为太原盆地的简单剪切模式.     

鄂尔多斯盆地东缘井区现今地应力特征与主控因素分析

近年来鄂尔多斯盆地东缘井区现今地应力研究匮乏.基于鄂尔多斯盆地若干区块地应力数据,通过计算拟合及数值模拟方法,深度分析了鄂尔多斯盆地东缘井区的现今地应力特征,讨论了岩石力学、裂缝走向和古地应场等地质因素对地应力分布的影响,提出了相应的开发建议.结果显示:鄂尔多斯盆地东缘井区地应力方向和大小分布具有一定规律性,在百米至千...     

Heterogeneous stretching, simple shear and basin development

The models of basin development which involve either homogeneous stretching of the whole lithosphere or displacement on a lithospheric-scale shear zone, are but two end members of a range of possible extensional models. The homogeneous extension model thins the lower lithosphere beneath the thinned upper crust and superimposes a thermal subsidence basin on the earlier fault bounded basin. The shear zone model offsets the zone of lower lithospheric stretching and thermal subsidence. It is more likely that the zones of upper and lower lithospheric stretching will be heterogeneous and patchy, but will often overlap in plan view. This will produce localised uplift and subsequent thermal subsidence within the faulted basin and may explain many of the anomalies between the various stretching estimates made using different structural, stratigraphic and geophysical techniques. The model which combines heterogeneous lithospheric stretching and associated simple shear may explain: (1) variations in dip of the major detachment zones in the large basins, (2) variations in types of strain on or beneath the detachment zones, (3) regional uplift of part of a basin, to erode the earlier fault blocks, and (4) the development of volcanism in basins with only low values of upper crustal extension. The zone of stretched lower crust and lithospheric mantle may lie beneath the centre of the zone of upper crustal stretching, or to one side. It may be linked to the upper crustal zone by faults which dip consistently in one direction, or by extensional systems which change their dominant dip direction with depth, pulling out the mid-crust as one or more wedges. Possible examples are discussed from the Basin and Range province and northwest European continental shelf.     

岩石圈流变性对拉张盆地构造热演化历史的影响

采用粘弹性动力学模型模拟研究了岩石圈流变性对拉张盆地构造热演化的影响. 模拟研究发现,盆地的构造热演化特征与盆、缘岩石圈强度对比相关,盆地岩石圈强度相对外缘岩石圈强度越弱,盆地沉降量越大,且在拉张结束与热沉降之间出现较大的基底抬升、热流持续高值;无论是初始岩石圈力学厚度、泊松比,还是下伏流体软流圈的负密度差,都是影响盆地构造热演化历史的因素;同时,拉张前断层的存在也是影响盆地基底形态的重要因素,其存在不仅会产生较大的基底落差,还会加深盆地中心的沉降.     

Volcano spacings and lithospheric/crustal thickness in the Archaean

There is a linear relationship between the spacing of Pliocene-Pleistocene volcanoes and the thickness of the lithosphere and attenuated crust in the East African rift valley. Assuming that the physical-chemical properties of the Archaean and Cenozoic lithosphere and crust were broadly similar, we use the spacing of volcanic centres in the Abitibi greenstone belt of southern Canada to determine lithospheric and crustal thickness in the Archaean. The abitibi volcanoes have been deformed and so have elliptical cross-sections. In order to arrive at their original form we have removed the effects of tectonic strain by two alternative mechanisms of pure and simple shear which give comparable results. A mean original volcano spacing of 84–88 km suggests that the lithsophere was 80–90 km thick and that the crust was probably 35–45 km thick in this greenstone belt about 2700 m.y. ago. The crustal values are comparable with those determined by geochemical parameters and are consistent with the suggestion that greenstone belts formed in extensional marginal basins between crustal-thickened continental masses, deep sections of which are now seen in Archaean high-grade regions.     

裂谷盆地构造-热演化模拟中几个问题的讨论

裂谷盆地的构造-热演化模拟是在岩石圈尺度计算裂谷盆地形成演化过程中的热历史和沉降史.拉张模型实现了构造和热的完美结合,在描述裂谷盆地沉降和热流演化方面取得了很大的成功.本文使用二维运动学模型,通过有限元方法,在拉格朗日坐标系下进行拉张背景下的构造热演化模拟,探讨了拉张模型中初始地壳、岩石圈厚度、软流圈对流、模型上边界对构造热演化的影响,以及载水和载沉积物两种情况下盆地侧翼抬升的差异.     

松辽盆地地壳精细结构研究

基于东北地区已有的宽频带流动台阵远震数据,利用波场延拓和分解的H-β网格搜索法,对松辽盆地的沉积层及地壳结构进行了深入分析。结果显示:松辽盆地的沉积层厚度为0.2—2.5 km,整体呈现中央坳陷区厚、边缘薄且西南地区最薄的分布特征;研究区地壳较薄,厚度介于24—34 km之间,其横向变化特征与沉积层厚度分布具有一定的对应性。依据沉积层和地壳的厚度计算了地壳伸展系数,其平均值接近于以往接收函数研究估测的岩石圈伸展因子。因此,本文推测松辽盆地在伸展构造过程中,其地壳和岩石圈的减薄以纯剪切模式为主。此外,松辽盆地具有较高的地壳平均波速比v_P/v_S,暗示盆地下方岩石圈地幔的减薄过程中可能存在岩浆的底侵作用。      

松辽盆地岩石圈减薄的深部动力学过程

松辽盆地作为东亚裂谷系的一部分,与华北克拉通一起经历了中生代岩石圈减薄的重大地质事件.对大陆岩石圈-软流圈状态和构造的整体认识,是研究大陆岩石圈减薄深部动力学过程的关键.在获得过松辽盆地的106个宽频和30个长周期大地电磁测深数据的基础上,完成测点数据二维偏离度、构造走向等计算与分析,进一步采用非线性共轭梯度算法,对TE和TM模式数据进行二维联合反演,获得了沿剖面的壳-幔电性结构,并依此构建了松辽盆地壳-幔结构模型.研究结果表明：（1）大兴安岭地区岩石圈厚度约为160 km,松辽盆地岩石圈厚度约为45 km,张广才岭岩石圈厚度在70~100 km之间,莫霍面与岩石圈底界面不呈镜像关系.软流圈整体表现为中、低阻异常,电阻率值在30 Ωm左右,其形态呈西倾约30°的蘑菇状异常,指示了软流圈物质上涌的形式,有别于软流圈垂直上涌的传统认识.（2）松辽盆地深部存在双层高导异常（电阻率小于5 Ωm）,上层为壳内高导层,呈"蛇"状分布,推断为岩浆底侵区,下层为幔内高导层,呈"哑铃"状,为软流圈上涌区.软流圈内存在两个"哑铃"状中、高阻异常,推断为拆沉的岩石圈地幔.具有冷的、高密度的下降物质流的堆积以及拆沉块体下插到两侧山岭是促使大兴安岭与张广才岭在中生代伸展环境中快速隆升重要原因;（3）松辽盆地经历了岩石圈减薄事件,与大兴安岭岩石圈厚度相比,松辽盆地岩石圈厚度减薄了近100 km,与东侧张广才岭相比减薄了70 km,而与中生代华北地台100 km的岩石圈厚度相比,减薄了近50 km,其经历了岩石圈伸展期、裂解期、拆沉期和增长期的动力学过程.     

Sedimentary basin development in the Archaean

The time history and magnitude of the subsidence in a sedimentary basin depends on the extent to which the lithosphere is thinned by stretching and on its original thickness. Hence the history and stratigraphic thickness of early Precambrian sedimentary basins, preserved as greenstone belts, should provide estimates of lithospheric thickness during the first half of the earth's history. Only the thickness of shallow-water sediments deposited without faulting is of relevance, and the best available estimates are compatible with all lithospheric thicknesses which have been suggested. The same is true of the estimates of the duration of the subsidence. Nonetheless radiometric dating can probably now provide estimates of the duration of the subsidence which are sufficiently accurate to constrain the models of the earth's thermal history if carried out for this purpose.     

Effects of finite rifting times on the development of sedimentary basins

Most thermo-mechanical models for the development of sedimentary basins have assumed that the rifting responsible for the formation of the basin occurred instantaneously and have examined the post-rift development of the basin. This assumption greatly simplifies the mathematical treatment, but is not in accord with what is found in nature, where 10-to 50-m.y. rifting events commonly accompany the formation of sedimentary basins and continental margins. The effects of a finite rifting time on the development of sedimentary basins are examined using an analytic technique which allows an arbitrary rifting history in both time and space and which considers the effects of both vertical and horizontal heat transfer. This technique allows the thermal structure of the lithosphere to be calculated throughout the rifting event and thus permits the subsidence history and surface heat flow of the developing basin to be traced.The effect of a finite-duration extension event is that heat is lost during rifting increasing the syn-rift subsidence at the expense of the post-rift. Lateral heat flow, which was not included in previous studies of the effect of finite rifting times, has a significant effect on the subsidence history, distribution of sediments and thermal history. In particular, the post-rift subsidence is decreased by more than 25% for a 20-m.y. rifting event and by more than 10–15% for a rifting event as short as 10 m.y. This will significantly decrease the subsidence rates in the post-rift stage and implies that inferences concerning the structure, development and thermal history of the basin derived from using “β-curves” to interpret backstripped subsidence can be greatly in error.Variations in syn-rift sediment accumulation and lithospheric thermal structure at the end of rifting resulting from different rifting histories can interact with other factors, such as the flexural response of the lithosphere to sediment loading, to affect the final width of the basin, the total amount of sediments that accumulate and the basin stratigraphy.     

Consequences of foreland basin development on thinned continental lithosphere: Application to the Aquitaine basin (SW France)

We present an analysis of the consequences of foreland basin development on thinned continental lithosphere, inherited from pre-orogenic phases of extension. Bathymetry at the transition from pre-orogenic extensional basin to foreland basin and compaction of pre-orogenic sediments contribute to the accommodation space for foreland basin sediments and thrust loads. In addition, the extension-induced transient thermal state of the lithosphere, results in ongoing thermal subsidence, and a flexural rigidity which changes through time. Quantitative modelling of the phase of extension and the foreland basin stage of the Aquitaine basin (southern France) shows that the inherited transient thermal state of the lithosphere contributes significantly to (1) the total foreland basin depth and width, (2) the post-compressional subsidence history, and (3) the cratonward onlap pattern. Accounting for the thermo-mechanical effects of pre-orogenic extension significantly reduces the estimates of both the flexural rigidity (30–43% for the Aquitaine basin) and the required topographic or thrust load (40% for the Aquitaine basin) at foreland basins. Emplacement of thrust loads below sea level, as expected in a pre-orogenic extensional basin setting, further reduces the required topographic load. This sheds light on the wide range of flexural rigidity values reported for continental lithosphere from foreland basin modelling studies, and explains, in many instances, the inferred ‘hidden load’ or subsurface load in flexural modelling studies at foreland basins. The present study has shown that pre-orogenic extension phases significantly affect the record of vertical motion and the stratigraphy of the Aquitaine basin and is probably important for foreland basin evolution in general.