龙门山断裂带三维滑动速率反演及其分段性研究

基于负位错模型,结合粒子群算法反演龙门山中央断裂段的三维滑动速率。反演结果表明,龙门山断裂带的现今构造运动整体而言为右旋逆冲断层,滑动速率较小,其运动特征具有显著的分段性。断裂带南段以逆冲为主,兼有左旋特征;在向北延展过程中逐渐转化为右旋走滑,且走滑分量逐渐加大;龙门山断裂带南北两端具有挤压特征,其中段显示一定的拉张。由此推断,龙门山断裂带现今构造活动,在青藏块体整体移动的影响下,还与其区域应力场和内部地壳结构有关。基于负位错模型,结合粒子群算法反演龙门山中央断裂段的三维滑动速率。反演结果表明,龙门山断裂带的现今构造运动整体而言为右旋逆冲断层,滑动速率较小,其运动特征具有显著的分段性。断裂带南段以逆冲为主,兼有左旋特征;在向北延展过程中逐渐转化为右旋走滑,且走滑分量逐渐加大;龙门山断裂带南北两端具有挤压特征,其中段显示一定的拉张。由此推断,龙门山断裂带现今构造活动,在青藏块体整体移动的影响下,还与其区域应力场和内部地壳结构有关。     

球体位错理论在2011年日本强震中的应用研究

利用球体位错理论计算了2011年日本强震产生的远场同震位移与应变,并利用GPS远场数据修正了该强震的总地震矩。结果表明：1）利用球体位错理论计算得到的理论水平位移场显示,垂直于发震断层的广大区域同震位移较大,位移矢量总体都指向震中地区,震中距约5 000千米的地方亦产生了3 mm以上的同震水平位移。理论位移与远场GPS观测结果具有良好的一致性;2）比较两个独立断层模型对应的理论同震位移场发现,震源西部地区远场位移总体上只有1%～4%的微小差异,而东部广大海域的差异则达到同震信号的6%～15%,震中周围差异更大。该差异表明,相对于震源仅局域覆盖的日本本土GPS观测数据对2011年日本强震的断层滑动分布模型的约束能力有限;3）依据中国及邻区的远场GPS同震观测数据修正2011年日本强震的总地震矩,把该地震释放的总能量约束在(3.24～4.96)×10 ²² Nm,相应的矩震级为Mw8.97～9.10;4）2011年日本强震在华北地区产生的同震应变与该区的长期应力变化背景场大体相反,表明该强震使华北地区的地壳产生了松弛效应。     

浅谈航摄底片压平质量对成图精度的影响

讨论了航摄底片压平检查时应满足的条件,对航摄底片压平精度超限产生的原因、压平精度超限在作业中的几种表现,以及底片压平精度超限在作业中的弥补办法等做了阐述.     

TIN向规则格网DEM转换的新算法

由TIN生成规则格网DEM是基于TIN的离散点数据栅格化的重要一步,在基于一种数学原理的基础上运用逆向思维提出了TIN向规则格网DEM转换的新算法,不用传统的分块和建立索引,而是通过逐个遍历三角形来判断格网节点位于哪一个三角形中并实现格网节点的插值。通过编程实现、测试该算法,证明它具有非常高的插值效率。     

基于Kriging方法的负偏态分布数据的空间插值研究

Kriging插值方法的前提是数据符合或基本符合正态分布的假设,或通过对非正态数据进行正态变换,使其满足要求。但对于拖尾的负偏态分布数据,正态变换方法无法奏效,若直接对数据进行Kriging插值,精度较低。文中在对样本数据深入分析的基础上,借助GIS平台,从不同透视角度对数据进行趋势分析,利用二次多项式模型对数据进行全局趋势拟合,并对随机的短程变异进行Kriging插值,选取不同的变异函数模型进行拟合比较,最终确定最优的模型参数,达到较为理想的插值结果。     

Observations and modelling of the travel time delay and leading negative phase of the 16 September 2015 Illapel,Chile tsunami

The systematic discrepancies in both tsunami arrival time and leading negative phase (LNP) were identified for the recent transoceanic tsunami on 16 September 2015 in Illapel, Chile by examining the wave characteristics from the tsunami records at 21 Deep-ocean Assessment and Reporting of Tsunami (DART) sites and 29 coastal tide gauge stations. The results revealed systematic travel time delay of as much as 22 min (approximately 1.7％ of the total travel time) relative to the simulated long waves from the 2015 Chilean tsunami. The delay discrepancy was found to increase with travel time. It was difficult to identify the LNP from the near-shore observation system due to the strong background noise, but the initial negative phase feature became more obvious as the tsunami propagated away from the source area in the deep ocean. We determined that the LNP for the Chilean tsunami had an average duration of 33 min, which was close to the dominant period of the tsunami source. Most of the amplitude ratios to the first elevation phase were approximately 40％, with the largest equivalent to the first positive phase amplitude. We performed numerical analyses by applying the corrected long wave model, which accounted for the effects of seawater density stratification due to compressibility, self-attraction and loading (SAL) of the earth, and wave dispersion compared with observed tsunami waveforms. We attempted to accurately calculate the arrival time and LNP, and to understand how much of a role the physical mechanism played in the discrepancies for the moderate transoceanic tsunami event. The mainly focus of the study is to quantitatively evaluate the contribution of each secondary physical effect to the systematic discrepancies using the corrected shallow water model. Taking all of these effects into consideration, our results demonstrated good agreement between the observed and simulated waveforms. We can conclude that the corrected shallow water model can reduce the tsunami propagation speed and reproduce the LNP, which is observed for tsunamis that have propagated over long distances frequently. The travel time delay between the observed and corrected simulated waveforms is reduced to <8 min and the amplitude discrepancy between them was also markedly diminished. The incorporated effects amounted to approximately 78％ of the travel time delay correction, with seawater density stratification, SAL, and Boussinesq dispersion contributing approximately 39％, 21％, and 18％, respectively. The simulated results showed that the elastic loading and Boussinesq dispersion not only affected travel time but also changed the simulated waveforms for this event. In contrast, the seawater stratification only reduced the tsunami speed, whereas the earth's elasticity loading was responsible for LNP due to the depression of the seafloor surrounding additional tsunami loading at far-field stations. This study revealed that the traditional shallow water model has inherent defects in estimating tsunami arrival, and the leading negative phase of a tsunami is a typical recognizable feature of a moderately strong transoceanic tsunami. These results also support previous theory and can help to explain the observed discrepancies.     

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Deriving 3D coseismic deformation field by combining GPS and InSAR data based on the elastic dislocation model

The density of GPS measurements is usually one of the key issues in resolving 3-D coseismic deformation field from integrating GPS and Interferometric Synthetic Aperture Radar (InSAR) measurements with pure mathematic interpolation methods An approach that combines the elastic dislocation model with the Best Quadratic Unbiased Estimator (BQUE) or a robust estimation method named IGG (Institute of Geodesy and Geophysics) is proposed to reconstruct 3-D coseismic deformation field, in which only a small amount of GPS data is needed to produce a reasonable initial 3-D coseismic deformation. Then the BQUE and IGG are used to weight the InSAR and GPS measurements to avoid computational issues caused by the negative variance problem and to decrease the impact from gross errors. The Wenchuan earthquake is used to test the proposed method. We find that the developed method makes it possible to use only a few GPSs and InSAR data to recover the 3-D coseismic deformation field, which offers extensive future usage for measuring earthquake deformation, particularly in some tectonically active regions with sparse GPS measurements.