南北带北段地壳上地幔密度与磁性结构

利用对应分析约束下的重磁联合反演方法,计算了南北带北段４条地震测深剖面的地壳上地幔的密度和磁化率物性参数。结果表明：①自上而下区内存在中新生界地层与下伏地层（０．１４￣０．３０ｇ／ｃｍ＾３）、中上地壳与下地壳（０．１０￣０．２０ｇ／ｃｍ＾３）和下地壳与上地幔顶部之间（０．３０￣０．４０ｇ／ｃｍ＾３）３个密度分界面;②区内磁性参数随深度增加而增大,浅部中新生界地层几乎无磁性,中上地壳磁化率一般为１０     

一秋龄性成熟中华绒螫蟹的生物学──1.外部形态特征及性腺变化

本文描述了一秋龄性腺成熟中华绒螯蟹（简称河蟹）的外部特征并与一秋龄未成熟及二秋龄成熟河蟹进行比较,同时给出了体重与壳宽的回归方程．保安湖的研究结果表明,对于一秋龄雌蟹,体重大于２９．８ｇ（壳宽为４．０３ｃｍ）全部成熟,而体重小于１３．１ｇ（壳宽为３．００ｃｍ）均不成熟,体重在１３、１－２９．８ｇ之间,既有成熟又有未成熟．对于一秋龄雄蟹,体重大于２６．０ｇ（壳宽３．９１ｃｍ）,全部成熟,而于１２．０ｇ壳宽２．６６ｃｍ）均未成熟,体重在１２．０－２６．０ｇ之间,既有成熟者又有未成熟个体．对一秋龄成熟河蟹成熟系数逐月变化的观察表明,在翌年３月份达到峰值,雌蟹为１２． ３２± １． ７５％,雄蟹为 ４． ２４± ０． ０６％;此后,性腺迅速退化,至翌年七月上旬,卵巢退变成细索状结构．己无完整的卵粒．     

多点冲击荷载作用下K6型单层球面网壳结构失效机理分析

为研究单层球面网壳结构在多点冲击荷载作用下的失效机理,在ANSYS/LS-DYNA中建立了60m跨度的Kiewitt 6型单层球面网壳结构的有限元模型,将整个网壳结构沿肋杆分成6个不同扇区,沿环杆分成5个不同环区,分别对网壳结构在同一环区和同一扇区受到多点冲击时的动力响应及冲击全过程能量传递的规律进行了分析研究。基于网壳结构失效变形特点,定义了多点冲击荷载作用下单层球面网壳结构的4类失效模式;根据整个冲击过程中能量的传递特点,揭示了单层球面网壳结构每类失效模式所对应的失效机理。     

1966年邢台6.8级地震的深总结背景

根据“八五”期间邢台地震区深部地震物理方法的综合探测研究成果，依据Ｐ波、Ｓ波联合解释和二维密度反演，并结合浅部构造和三维应力场数值模拟计算等资料，进行综合分析研究。以１９６６年邢台６．８级地震为例，揭示了邢台地震区的孕震发震过程，邢台地震区的学位可结构和介质结构；（１）中、下地壳内分布有北东向高角度深断裂、深断裂两则出现明显的波速比异常。（２）中地壳有低速高层和密度不均匀异常。（３）上地壳底部有滑     

天山造山带地壳结构与构造──乌鲁木齐─库尔勒地震转换波测深剖面

沿乌鲁木齐－库尔勒３５０余公里长的测线上完成了穿越天山的地震转换波野外观测，得出天山造山带的深部构造剖面图和壳内Ｐ，Ｓ波速度结构模型．天山的结晶地壳可分为４层，各层的速度分别是：Ｖｐ值为５．９，６．３，６．６，６．９ｋｍ／ｓ；Ｖｓ值为３．２，３．５，３．７，３．９ｋｍ／ｓ。上地幔顶部的波速：Ｖｐ值为８．１０ｋｍ／ｓ。Ｖｓ值为４．６ｋｍ／ｓ。天山地区的地壳厚度为４２－５６ｋｍ，中天山最厚，达到５０－５６ｋｍ。地壳中部存在低速透镜体。探测结果表明，天山大地构造可分为北天山、中天山和南天山３个区，其地壳深部构造特征各不相同。用颤动构造理论来解释天山造山带的形成机制和演化较板块构造理论更为合理。     

天山造山带地壳结构与构造──乌鲁木齐─库尔勒地震转换波测深剖面

沿乌鲁木齐－库尔勒３５０余公里长的测线上完成了穿越天山的地震转换波野外观测，得出天山造山带的深部构造剖面图和壳内Ｐ，Ｓ波速度结构模型．天山的结晶地壳可分为４层，各层的速度分别是：Ｖｐ值为５．９，６．３，６．６，６．９ｋｍ／ｓ；Ｖｓ值为３．２，３．５，３．７，３．９ｋｍ／ｓ。上地幔顶部的波速：Ｖｐ值为８．１０ｋｍ／ｓ。Ｖｓ值为４．６ｋｍ／ｓ。天山地区的地壳厚度为４２－５６ｋｍ，中天山最厚，达到５０－５６ｋｍ。地壳中部存在低速透镜体。探测结果表明，天山大地构造可分为北天山、中天山和南天山３个区，其地壳深部构造特征各不相同。用颤动构造理论来解释天山造山带的形成机制和演化较板块构造理论更为合理。     

利用接收函数探讨新疆几次中强地震的地壳孕育深度

在分析2009～2012年新疆地区的远震P波接收函数过程中,发现部分台站的接收函数中存在清晰且能量较强的壳内间断面转换波。本文分别利用接收函数中的壳内间断面和莫霍面转换波,联合接收函数H-κ叠加方法和时间窗滑动方法,分析了2009～2012年新疆6次中强地震震中周围的7个地震台站下方的地壳和上地壳(壳内间断面上方地壳)介质泊松比在地震前后随时间的动态变化情况。结果显示:乌苏、于田和独山子3个地震台站的地壳介质泊松比在对应的3次中强地震前后出现了较为明显且持续的下降过程,下降幅度大于均值误差,变化形态特征呈"V"字型(乌苏台呈双"V"字型),地震发生在"V"字形成的尾端,但其上地壳介质泊松比在地震前后没有出现明显低值异常变化;其他4个地震台站下方的地壳和上地壳介质泊松比在地震前后没有观测到明显低值异常。根据观测结果,推测3次中强地震前后地壳介质泊松比出现低值异常主要源于中下地壳,地壳孕育深度位于中下地壳。     

珠江三角洲芦苞—佛山—中山—三乡断面的地壳结构——密集台阵勘探新成果

为了研究珠江三角洲核心地区中深部地壳结构,在芦苞—佛山—中山—三乡地区开展了密集台阵勘探工作,使用接收函数方法处理反演,获得珠江三角洲核心地区40 km以浅Vs速度结构.结合研究区的地质、重力异常特征对反演成果分析获得初步成果:珠江三角洲地区地壳结构可分为上地壳、中地壳、下地壳和上地幔四个大层位,上地壳厚度在临海一侧变厚,在中山三乡镇一带,厚达14 km;莫霍面隆起、上地幔物质侵入下地壳和高密度岩浆侵入上地壳这个三个因素共同导致研究区重力异常高;获得了沿线中深部断裂构造空间展布特征信息,速度结构和断裂构造具有较好的相关性;沿测线地壳在15～20 km深的深度上不存在低速层;三水盆地基底深度在3 km左右,与该地区沉积层厚度一致;莫霍面深度北深南浅,深度在27.5～30 km之间,其波速特征明显,由3.6 km/s突变为4.1 km/s.     

用数值模拟方法评估华北北部地震危险性

根据华北北部地区深浅部地质特征建立地质模型,采用含位错面的三维粘弹性有限单元方法,在反演断层深部滑动速率的基础上计算区域内有效应力和应变能密度随时间的变化。由数值模拟结果估计华北北部的地震危险性,提出了 ３ 个潜在震源区：张家口及以北地区,震级上限为 ６ 级,孕震层在上地壳下部;延怀盆地,震级上限为 ７ 级,孕震层在中地壳;阳原盆地,震级上限为６ 级,孕震层在下地壳上部     

腾冲火山及邻区速度结构的三维层析成象

利用１９８４～１９９８年新间期间发生在腾冲火山及邻区３０个台站记录的数知个地震的Ｐ波资料,采用地震层析成象法重建了腾冲火山及邻区地壳、上地幔不同深度的三维速度结构层析成象图。结果给出,在腾冲火山区下面地壳内约３～９ｋｍ存在低速带,扰动量达－２０％;１０～１５ｋｍ深度为高波速带,扰动量达７．３％;１６～２４ｋｍ深度为低波速带。扰动量达－９．１％;２５～４０ｋｍ为波速带,扰一达１０％;大于莫霍面深度（     

多波多分量高斯束叠前深度偏移

本文对基于弹性波动理论的多波多分量高斯束偏移进行了完整且详细的分析和公式推导,实现了3D空间多分量(矢量)波场的直接成像.由于当前多数基于弹性波动方程的偏移方法只是假设应力边界条件为自由地表边界条件,这种假设不符合垂直地震剖面(VSP)和海底电缆(OBC)等地震数据.为此本文详细分析了实际应用中常见的三种弹性各向同性介质模型的应力边界条件:自由空间、海底和自由地表模型.在上行传播假设情况下,获得了应力边界条件与位移边界条件的关系式.在此基础上,准确推导了3D多波多分量高斯束波场延拓和偏移成像公式,并在偏移过程中实现了完整的多波型自动分离.由于常规的互相关成像条件不适用于矢量波场成像,本文引用了散度/旋度互相关成像条件.通过约定PS转换波的正向旋转方向解决了3D空间PS成像极性翻转问题.利用2D和3D模型数据偏移成像验证了我们所提出的多波多分量高斯束偏移方法的可行性.     

基于黏弹性边界的地震动输入方法和边界条件选择研究

针对地下工程抗震分析中边界条件和地震动输入方式选择问题,对一地下半无限体模型在一剪切波垂直入射条件下进行不同边界条件和不同地震动输入方法的算例试算。结果发现:两侧采用竖直向位移约束、底部采用黏弹性边界、并在模型底部用等效节点力输入地震动的方法,与三边均采用黏弹性边界条件和三边均采用等效节点荷载输入地震动的方法可以获得同样的结果。该方法易于在ANSYS中通过APDL编程实现,可为地下工程抗震分析中黏弹性边界的使用提供便利。     

On the use of horizontal acoustic Doppler profilers for continuous bed shear stress monitoring

Continuous monitoring of bed shear stress in large river systems may serve to better estimate alluvial sediment transport to the coastal ocean.Here we explore the possibility of using a horizontally deployed acoustic Doppler current profiler(ADCP) to monitor bed shear stress,applying a prescribed boundary layer model,previously used for discharge estimation.The model parameters include the local roughness length and a dip correction factor to account for sidewall effects.Both these parameters depend on river stage and on the position in the cross-section, and were estimated from shipborne ADCP data.We applied the calibrated boundary layer model to obtain bed shear stress estimates over the measuring range of the HADCP.To validate the results,co-located coupled ADCPs were used to infer bed shear stress,both from Reynolds stress profiles and from mean velocity profiles. From HADCP data collected over a period of 1.5 years,a time series of width profiles of bed shear stress was obtained for a tidal reach of the Mahakam River,East Kalimantan,Indonesia.A smaller dataset covering 25 hours was used for comparison with results from the coupled ADCPs.The bed shear stress estimates derived from Reynolds stress profiles appeared to be strongly affected by local effects causing upflow and downflow,which are not included in the boundary layer model used to derive bed shear stress with the horizontal ADCP.Bed shear stresses from the coupled ADCP are representative of a much more localized flow,while those derived with the horizontal ADCP resemble the net effect of the flow over larger scales.Bed shear stresses obtained from mean velocity profiles from the coupled ADCPs show a good agreement between the two methods,and highlight the robustness of the method to uncertainty in the estimates of the roughness length.     

An analysis of shear stress distribution in circular channels with sediment deposition based on Gene Expression Programming

Knowledge of the boundary shear stress distribution in channels is important because it is a key factor affecting on erosion and sedimentation rates. The presence of sediment deposits in sewers is often reported during operation, and circular channels are frequently used in sewer networks. Gene expression programming(GEP) is applied in this study to determine an equation for evaluating the shear stress distribution along the wetted perimeter of a circular channel with a flat bed, because of the presence of sediment on the bed. In view of the parameters affecting the shear stress distribution, five dimensionless parameters are applied to develop six GEP models to be used with 905 experimental data. The impact of the shear stress parameters is studied using the six GEP models and by dividing the wetted perimeter into wall and bed sections. Two equations are extracted from the GEP models' output to estimate wall and bed shear stresses. The best model results are compared with a well-known equation based on the entropy concept. The GEP model predictions of wall and bed shear stresses are very similar to the experimental outcomes, whereas the entropy-based model overestimates the shear stress distribution.The proposed GEP models demonstrate superior performance in estimating the shear stress distribution with a mean absolute percentage error(MAPE) of 3.79% compared to an existing equation with MAPE of 9.52%.     

Mechanical analysis of en echelon structure and its significance of controlling earthquakes

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FLOW FIELD IN SCOURED ZONE OF CHANNEL CONTRACTIONS

Experiments were conducted in a laboratory flume to measure the two-dimensional turbulent flow field in the scoured zone of channel contractions under a clear-water scour condition. The Acoustic Doppler Velocimeter (ADV) was used to detect the flow field at different vertical lines along the centerline of uncontracted (main channel) and contracted zones of the channel. The distributions of time-averaged velocity components, turbulent intensity, turbulent kinetic energy, and Reynolds stresses are presented in nondimensional graphical form. The bed shear stresses are computed from the measured Reynolds stresses being in threshold condition within the zone of contraction where bed was scoured. The data presented in this paper would be useful to the investigators for the development of kinematic flow model and morphological model of scour at a channel or river contraction.     

3-D spherical shell modeling of mantle flow and its implication for global tectogenesis

In order to study the relationship between mantle flow and global tectogenesis, we present a 3-D spherical shell model with incompressible Newtonian fluid medium to simulate mantle flow which fits the global tectogenesis quite well. The governing equations are derived in spherical coordinates. Both the thermal buoyancy force and the self-gravitation are taken into account. The velocity and pressure coupled with temperature are computed, using the finite-element method with a punitive factor. The results show that the lithosphere, as the boundary layer of the earth's thermodynamic system, moves with the entire mantle. Both its horizontal and vertical movements are the results of the earth's thermal motion. The orogenesis occurs not only in the collision zones at the plates' boundaries, but also occurs within the plates. If the core-mantle boundary is impermeable and the viscosity of the lower mantle is considerable, the vertical movement is mostly confined to the upper mantle. The directions of the asthenospheric movements are not fully consistent with those of the lithospheric movements. The depths of spreading movements beneath all ridges are less than 220 km. In some regions, the shear stresses, acting on the base of the lithosphere by the asthenosphere, are the main driving force; but in other regions, the shear stresses are the resisting force.     

水平应力作用下套管井不同胶结状况导波的声弹效应

油田的套管完井常伴有异常地应力的作用,对于套管井,井孔-套管-水泥环-地层组合的系统使井周的应力集中更为复杂.为认识地应力作用下不同胶结状态的套管井导波声弹效应,本文基于非线性声学理论,实现了受应力作用不同胶结状态套管井井周应力和径向横波速度计算与分析;采用摄动求解推导了套管井导波的声弹性方程,模拟并分析由应力引起不同胶结状态套管井斯通利波、伪瑞利波、弯曲波相速度的变化.研究结果表明:不同胶结状态会改变井周的应力分布,当界面出现滑移时井周地层中的应力集中有所增强,从而影响导波的声弹效应.本文的研究结果为地应力作用的套管井的声场特性提供认识和理论依据.     

Apparent stress and stress drop for intraplate earthquakes and tectonic stress in the plates

The magnitude of shear stress in the lithosphere is bounded from below by the apparent stress and stress drop during intraplate earthquakes. Apparent stresses and stress drops for a number of mid-plate earthquakes are calculated from the earthquake magnitude, SH wave amplitude spectra, and estimates of the length of the fault zone. Apparent stresses vary between 0.1 and 2 bars, ifm _b is used as a measure of seismic energy, and stress drops lie between 2 and 70 bars. There is no systematic difference in either apparent stress or stress drop between these intraplate events and typical plate boundary earthquakes. These bounds on intraplate shear stresses are consistent with the inference from current models of plate tectonic driving forces that regional stress differences in the plates are typically on the order of 100 bars. The highest stress drops measured for midplate earthquakes under this model represent nearly total release of local tectonic stress.