用远震接收函数反演福建地区宽频带台站下方莫霍界面深度

收集福建省“九五”数字地震遥测台网中8个宽频带台站的远震波形资料,应用接收函数的研究方法计算各个台站下方的接收函数。采用非线性的反演方法获得这些台站下方的S波速度结构．确定这些台站下方莫霍界面深度的分布情况。分析得到的反演结果,福建地区莫霍面的起伏不大．平均的地壳厚度约为32km。在0～2km之间均存在一层低速层,这与地表覆盖着一层松散的沉积层是相对应的。内陆地区台站附近莫霍界面深度较沿海地区略高,沿海台站的莫霍界面深度北部略高于南部。     

福建近岸海域滨海断裂的应力分析

福建东南沿海地区曾发生多次强震。本文利用该区1604～1989年的47次地震的震源机制资料,采用力轴张量计算法推算了该区应力主轴方向,结果与其他文献给出的主压应力方向相符,即北西西-南东东向。在此基础上,得到最大剪切应力平面的走向和倾角。讨论了最大剪切应力平面与福建沿海近岸海域中存在的滨海断裂（牛山岛-兄弟屿断裂）的位置关系。从应力分析的角度初步探讨了滨海断裂带上地震活动由北向南增强的原因。     

北京及邻区现代微震重新定位及其构造含义

本文采用Ｐｏｗｅｌｌ直接搜索定位方法对北京西北地区（３９°－４１°Ｎ，１１４°－１１７°Ｅ）１９７９—１９９２年３月发生的３４８个地震重新定位。通过震相到时的复核和补充、定位速度结构模型的修定以及定位程序的改进等措施，改善了定位效果。结果表明，重新定位后给出震源深度的地震数从原来的１３２个增至３１３个；定位结果均方根残差的均值从０．８０±０．４０ｓ降至０．４５±０．１８ｓ；各台Ｐ波到时残差下降；有近１０％的地震震中位置移动了１０ｋｍ以上，它们多位于北京地震遥测台网边缘地区。重新定位后的地震震中集中分布于怀安、宣化、怀来、琢鹿等山间盆地内部并与盆地边缘断裂有关。此外，地震还分布于山区和平原的交界地带。     

汶川8.0级地震前龙门山断裂带的地震活动性和构造应力场特征

研究了2008年5月12日汶川8.0级地震前龙门山断裂带及其附近地区的地震活动.利用区域地震台网和流动测震台的数字地震波资料,测定了震源机制解.结果表明,震中所在的龙门山断裂带震前地震活动平稳,未出现显著异常增强或平静现象.根据汶川8.0级地震前地震活动求出的震源机制解,其主压应力P轴方位为WNE——ESE向,震源断层面呈NE向与NW 向两组节面走向.其中NE向节面呈N50deg;——70deg;E,断面倾角均陡,达60deg;——70deg;,震源力学作用方式多呈逆倾型,少部分呈走滑型．震前地震活动呈现的主压应力方位、震源断面走向及其错动类型,与汶川8.0级地震给出的解是一致的.巨大地震发生前沿龙门山断裂带微破裂呈现的平均应力场与主震一致．起始破裂区东侧20km内是紫坪铺水库水域区,这一区域发生小震活动增加的现象处于水库放水的卸载阶段.本文研究了汶川8.0级地震起始破裂区附近的小震活动,其震源参数表明,震源位于8.0级地震之上的5——14km深度,其震源参数与8.0级地震给出的解也是一致的．      

二阶精度广义非线性全局最优的偏移速度反演方法(英文)

如何快速、精确地利用叠前深度偏移进行偏移速度分析是勘探地震学的一项重要研究内容,针对该问题,本文提出一种二阶精度广义非线性全局最优的偏移速度反演方法。我们将首先去掉速度模型修正量与成象深度差呈线性关系的假设,推导出具有二阶精度的速度模型修正量计算公式,使每一次迭代得到的速度模型尽可能地接近实际模型;然后采用广义非线性反演方法反演获得对所有道集的全局最优的速度模型修正量,不仅极大地加快了收敛速度,而且反演过程中陷入局部极小的可能性也减小了。理论模型和Marmousi模型的处理结果表明:本方法精度高、处理速度快,提高了偏移速度分析方法的实用性和对复杂构造成像的准确性。     

Velocity structure of uppermost mantle beneath North China from Pn tomography and its implications

20301 Pn arrival time data are collected from the seismological bulletins of both national and regional seismic networks. Pn travel time residuals are tomographically inverted for the Pn velocity structure of uppermost mantle beneath North China. The result indicates that the average Pn velocity in North China is 7.92 km/s, and the velocity varies laterally from ?0.21 to +0.29 km/s around the average. The approximately NNE trending high and low velocity regions arrange alternatively west-eastward. From west to east we can see high velocity in the middle Ordos region, the Shanxi graben low, the Jizhong depression high, the west Shandong uplift and Bohai Sea low, and the high velocity region to the east of the Tanlu fault. In the southern boundary zone of the North China block, except for the high velocity in the Qingling Mountains region, the velocity is generally lower than the average. Obvious velocity anisotropy is seen in the Datong Cenozoic volcanic region, with the fast velocity direction in NNE-SSW. Notable velocity anisotropy is also seen around the Bay of Bohai Sea, and the fast velocity directions seem to show a rotation pattern, possibly indicating a flow-like deformation in the uppermost mantle there. The Pn velocity variations show a reversed correlation with the Earth's heat flow. The low Pn velocity regions generally show high heat flow, e.g., the Shanxi graben and Bohai Sea region. While the high Pn velocity regions usually manifest low heat flow, e.g., the region of Jizhong depression. This indicates that the Pn velocity variation in the study region is mainly aroused by the regional temperature difference in the uppermost mantle. Strong earthquakes in the crust tend to occur in the region with the abnormal low Pn velocity, or in the transition zone between high and low Pn velocity regions. The earthquakes in the low velocity region are shallower, while that in the transition zone are deeper.     

Experimental assessment and prediction of temporal scour depth around a spur dike

Spur dikes are river training structures that have been extensively used worldwide for towards enhancing flood control and the stability of embankments and riverbanks.However,scour around spur dikes can be a major problem affecting their stability and hydraulic performance.The precise computation of temporal scour depth at spur dikes is very important for the design of economical and safe spur dikes.This study focuses on experimentally assessing the temporal variation of scour depth around a vertical wall spur dike and identifying the parameters,which mostly influence spur dike performance for a channel bed surface comprised of sand-gravel mixtures.In the current study,the authors did physical experiments in a flume based study to obtain new data,aimed at deriving a new predictive model for spur dike scour and comparing its performance to others found in the literature.It was found that the dimensionless temporal scour depth variation increases with an increase in(i)the threshold velocity ratio,(ii)the densimetric Froude number of the bed surface sediment mixture,(iii)the flow shallowness(defined as the ratio of the approach flow depth,y,to the spur dike’s transverse length,l),and(iv)the flow depth-particle size ratio.It is also concluded that the temporal scour depth variation in the sediment mixture is influenced by the non-uniformity of sediment and decreases with an increase in the non-uniformity of the sediment mixture.A new mathematical model is derived for the estimation of temporal scour depths in sand-gravel sediment mixtures.The proposed equation has been calibrated and validated with the experimental data,demonstrating a good predictive capacity for the estimation of temporal scour depth evolution.     

Lateral variation in Moho depth around the southern Tanlu fault zone and its adjacent area

We estimated Moho depth beneath the southern Tanlu fault zone and its adjacent area using common-conversion-point(CCP)stacking of receiver fun-ctions,which were computed from teleseismic records of the CEArray.Our estimated Moho depth matches well with 2-D profiles derived from active-source deep seismic reflection surveys,suggesting that the calculated the Moho depth map is likely accurate beyond the 2-D profiles.Overall,the estimated Moho depth map showed a high spatial correlation with tectonic provinces,i.e.,Moho topographic boundaries are in good agreement with geological boundaries.Beneath the Dabie orogenic belt and the mountainous areas in southern Anhui Province,the Moho lies relatively deep,and there is an obvious difference in Moho depth between the two sides of this segment of the Tanlu fault.We further selected four depth profiles with dense instrumentation to show Moho depth changes across different tectonic blocks in the study area.We saw two step-like changes in Moho depth beneath the Xiangfan-Guangji and Gushi-Feizhong,which run parallel along the WNW-ESE direction and delineate the southern and northern bounds of the northern Dabie orogenic belt,which is likely the suture zone between the North China Block and South China Block.Crust beneath the northeast corner of the study area is significantly thinner than other areas,which is consistent with the crustal detachment model proposed for suturing between the North and South China blocks in the region east to the Tanlu fault.     

地-空瞬变电磁法电阻率成像研究与应用

地-空瞬变电磁法（Semi-airborne transient electromagnetic,SATEM）凭借适应能力强、探测深度大、实时性强等特点,适用于湖泊、沼泽、山区等地形复杂地区观测.SATEM接收数据量大、精度要求高,传统成像方法基于地面视电阻率计算未考虑飞行高度,开展SATEM的高精度快速成像研究对实际运用有重要作用.针对SATEM中电性源发射装置感应电流分布,接收装置设置于空中以及两者不在相同平面的特点,本文考虑横向、纵向感应电流差异,飞行高度对视电阻率影响等因素,提出电性源SATEM电阻率成像方法.首先,基于电性源瞬变电磁场感应电流分布特征及各分量空间分布、扩散特性分析,推导出基于均匀半空间磁场与感应电压解析解,然后定义了电性源地-空瞬变电磁法早期、晚期、全期视电阻率;最后根据对感应电流分布分析定义了横向分量和纵向分量的成像深度,并研究了成像深度受飞行高度、发射磁矩、偏移距、偏移角度的影响;对煤炭采空区的实测结果表明,利用本文提出的电阻率成像方法可以更加精确定位目标体位置.

     

2021年3月19日西藏比如MS 6.1地震总结

2021年3月19日西藏比如MS 6.1地震发生在班戈—安多地区的安多盆地南缘断裂附近,震源机制解反演结果显示,本次地震为近东西走向断层产生正断兼走滑型错动的结果,与区域构造特征一致;截止至4月15日,地震序列跟踪发现,主震与余震震级差为1.4,主震释放能量占序列的98.96％,表明6.1级主震释放了此次地震序列的绝大...