THE DEPTH OF MOHO INTERFACE AND CRUSTAL THICKNESS IN SICHUAN-YUNNAN REGION,CHINA

By using moving average method to separate Bouguer gravity anomaly field in Sichuan-Yunnan region, we got the low-frequency Bouguer gravity anomaly field which reflects the undulating of Moho interface. The initial model is obtained after seismic model transformation and elevation correction. Then, we used Parker method to invert the low-frequency Bouguer gravity anomaly field to obtain the depth of Moho interface and crustal thickness in the area. The results show that the Qinghai-Tibet block in the northwest of the study area deepens and thickens from the edge to the interior, with the depth of Moho interface and the crust thickness of about 52~62km and 54~66km, respectively. The depth of Moho interface in Sichuan Basin is about 38~42km. In Sichuan-Yunnan block, the depth of Moho interface is about 42~62km from southeast to northwest. Beneath the West Yunnan block, west of the Red River fault zone, the Moho depth is about 34~52km from south to north. The Longmen Mountains and Red River fault zone are the gradient zone of the Moho depth change. Along the Red River fault zone, the depth difference of Moho interface is increasing gradually from north to south. No obvious uplift is found on the Moho interface of Panzhihua rift valley. The depth of Moho interface distribution in Sichuan and Yunnan is obviously restricted by the collision between the Indian plate and the Eurasian plate and the lateral subduction of the Indo-China peninsula. The mean square error of the depth of Moho interface is less than 1.7km between the result of divisional density interface inversion and artificial seismic exploration. At the same time, we compared the integral with divisional inversion result. It shows that:in areas where there is obvious difference between the crust velocity and density structure in different tectonic blocks, the use of high resolution seismic exploration data as the constraints to the divisional density interface inversion can effectively improve the reliability of inversion results.     

首都圈地区Pb震相典型特征与康拉德界面研究

Pb震相是近震震相中的一个重要震相.关于Pb震相典型特征的总结和分析,对指导区域台网工作人员如何识别该震相,丰富台网观测报告震相产出,提高地震定位精度和确定康拉德界面等相关研究具有重要意义.但由于识别困难,国内很少有系统进行有关Pb震相的识别和研究工作.本研究采用首都圈地区高密度台网2009-2015年记录到的369个ML≥2.5地震事件的波形资料,重新分析震相并识别出1153条Pb震相.基于震相资料,利用时频分析、多项式拟合、射线分析、最小二乘法、联合反演、理论走时计算等方法进行研究,并在结合前人研究结果的基础上,我们得出:在首都圈及邻区,在肉眼可识别时频域内的特征来看,通常容易识别的Pb的振幅或频率高频部分相对比初至Pn和Pg大或高,也有振幅变小或者频率变化不明显的情况,这可能与震源机制、台站方位、场地响应、仪器类型等方面有关.时频分析、功率谱密度和肉眼识别分析的结果表明,P波的主要能量集中在相对低频部分,Pn,Pb,Pg,PmP四种震相(本研究以后提到的震相顺序只考虑这四种震相)有很强的共性,区别在于传播路径上的不同,频率或观测记录周期上的小幅度差别.在Pg作为初至波时,Pb震相的低频主频部分与Pg震相的低频主频部分带宽差不多(受到包含Pg震相的影响),但是高频主频部分频率更高,Pb到时在Pg之后,PmP之前.Pn作为初至波时,Pn震相低频主频部分带宽比Pb宽,但是Pb高频主频部分频率相对更高,Pb在Pn之后,在Pg之前.鉴于震源深度对Pb到时顺序的影响,及其在定位结果中精确度最差的情况,在震中距约在80~140km范围内时,得考虑区域地壳厚度横向不均匀、震中距、震源深度等情况并结合波形特征,来判定Pb是否为初至震相.Pb震相在康拉德界面的平均传播速度约为7.0km·s^-1,康拉德界面平均深度约为23km.Pb射线的分布情况直接证明了康拉德界面在首都圈地区的分布是连续的.基于本研究利用Pg,Pb,Pn,PmP震相走时联合反演所得模型计算的理论走时结果和实际观测结果一致进一步证明了我们结果的可靠性.     

长江中下游典型湿地沉积物-水界面硝酸盐异养还原过程

反硝化(Denitrification,DNF)和硝酸盐异化还原为氨(Dissimilatory Nitrate Reduction to Ammonium,DNRA)是硝酸盐异养还原的2个主要途径.反硝化被认为是彻底去除水体氮负荷的主要过程;而硝酸盐异化还原为氨则将水体中的硝态氮转化为氨氮.2个过程均以硝酸盐为电子受体,并存在相互竞争关系.这2个过程的研究对理解湿地氮转化以及指导湿地氮污染修复具有重要意义.运用无扰动沉积物柱样流动培养、15NO-3-N同位素示踪实验,并采用氨氧化-膜接口质谱仪联用(OX/MIMS)测定氨氮同位素产物的方法,对鄱阳湖碟形湖湿地、巢湖重污染河流湿地、巢湖重污染湖泊湿地3种类型湿地沉积物-水界面的硝酸盐异养还原过程进行研究,结果表明存在显著差异.3种类型湿地DNF速率的范围为(6.36±2.57)~(99.98±14.05)μmol/(m2·h),DNRA速率的范围为(0.51±0.45)~(79.82±6.08)μmol/(m2·h).在3种类型湿地中,随着氮污染程度加重,DNF和DNRA速率均显著增加,且DNRA过程在总的硝态氮异养还原中所占的比重不断增大,说明较高的硝酸盐负荷、较高的沉积物有机质含量更有利于DNRA过程的竞争.而对反硝化方式的进一步研究发现,巢湖重污染河流、湖泊湿地主要以非耦合反硝化为主导过程,而鄱阳湖碟形湖湿地则更倾向于以硝化过程耦合控制的反硝化为主.     

湖泛水体沉积物-水界面Fe2+/ΣS2-迁移特征及其意义

湖泊水底Fe~(2+)和ΣS~(2-)浓度的快速增加是湖泛暴发最早发生于沉积物-水界面的主要前提,缺氧环境下水底扩散层附近Fe~(2+)和ΣS~(2-)的迁移是其在沉积物-水界面处稳定积累的重要原因.以蓝藻聚积水体沉积物-水界面为研究对象,应用湖泊过程模拟装置及间隙水被动采样等技术,重点研究了间隙水和底层上覆水中Fe~(2+)和ΣS~(2-)的垂向分布特征,并定量估算了二者的扩散通量及迁移方向.结果表明:湖泛样品水体沉积物-水界面处于典型的还原性环境,表层沉积物间隙水中Fe~(2+)和ΣS~(2-)浓度显著高于对照样品,二者在表层沉积物中积累趋势明显.湖泛水体沉积物-水界面处Fe~(2+)释放通量较高,表现出较强烈的自沉积物向上覆水方向的释放能力;而湖泛样品ΣS~(2-)在沉积物-水界面处释放通量为负,迁移方向为自上覆水向沉积物扩散.Fe~(2+)和ΣS~(2-)在湖泛水体沉积物-水界面处不同的迁移特征证明:缺氧/厌氧条件下,湖泊水体表层沉积物间隙水中高浓度Fe~(2+)向上覆水的扩散为湖泛致黑物质的形成提供了重要的物质基础;底层上覆水及界面水中SO~(2-)4在表层沉积物中被还原,为终端还原产物ΣS~(2-)为湖泛致黑物质的形成提供了另一重要物质来源.     

基于RS232接口的温度传感器自动检定系统设计

针对目前省级气象计量实验室配备的测试设备大多具有RS232可编程接口,为了提高温度传感器的检定效率,研究了SR253型温控器、精密测温仪和常用的3种扫描采集器等设备的串口通信协议,在VB6.0开发平台下结合SQL Server 2000数据库编程实现了温度传感器的自动检定。试验结果表明:系统不仅性能可靠、操作方便,通用性较高,明显提高了检定效率,而且避免了手动检定时的人为影响因素,保证了检定数据可靠性。     

非一致激励条件下工程场地地震动相干函数的数值模拟--Ⅱ分析方法的应用

在文《非一致激励条件下工程场地地震动相干函数的数值模拟———Ⅰ分析原理和方法》中,通过将随机振动的虚拟激励原理与工程波动理论散射问题的求解方法相结合,提出了开放系统中非一致激励条件下工程场地地震动随机场的数值模拟方法。本文将建议方法应用于具有非一致随机激励的复杂工程场地的地震动相干函数分析之中,讨论了受局部场地条件影响的地震动相干函数的若干特征。     

混凝土结构CFRP加固界面粘接质量DSSPI无损检测研究

本文将数字错位散斑技术引入CFRP加固混凝土界面粘接质量的检测。对预制缺陷模型检测的结果表明,该方法能够迅速准确地对CFRP加固粘接质量作出检测和评价,为混凝土结构加固界面粘接质量无损诊断提供一种新思路。     

Dynamics of attached bacteria at the water-sediment interface in a mesotrophic swampy bog of Japan

The population dynamics of attached bacteria at the water-sediment interface were studied in a mesotrophic swampy bog, Matsumi-ike, near Tsukuba, Japan. The density of attached bacteria was higher at the sediment boundary layer than in the water column, and low inside the sediment (deeper, than 10 mm below the sediment surface) throughout the year. The density of bacteria attached on the glass slide was highest during spring when the source of organic matter in the water column was mainly withered cattail, and gradually decreased toward summer, while the phytoplankton became the dominant source of organic matter in the water column. The epibacterial populations in the water column and at the boundary showed almost the same seasonal fluctuation in attachment and detachment rates. However, bacterial growth rates did not show the same seasonal fluctuation, and annual average growth rates on the glass slides were all lower than that of bacterioplankton (free-living bacteria in water) in the water column.     

Numerical computations of resonant sloshing using the modified isoAdvector method and the buoyancy-modified turbulence closure model

Sloshing is an interfacial-flow phenomenon which brings two challenges on how to locate the position of the interface and avoid the unphysical motion of the interface. In order to locate the the position of the interface, a new geometric Volume-of-Fluid (VOF) method called isoAdvector is adopted to pursue a sharp interface. Aiming to make the isoAdvector method compatible with the dynamic mesh adopted to handle the tank motion, the motion-flux correction is introduced, and a moving-velocity correction for face-interface intersection line (FIIL) is proposed. An approximation formula is adopted to effectively reconstruct the moving-velocity field of the meshes at each cell center based on the motion fluxes on each cell face. In order to avoid the unphysical motion of the interface due to the excessive turbulence level in the transition region at the interface, the buoyancy-modified k − ω SST model is adopted. The numerical results of wave elevations and forces are compared with the experiments. The comparisons suggest that (i) the moving-velocity correction for FIIL is important to update the volume fraction; (ii) the modified isoAdvector method can capture the the position of the interface more accurately than the algebraic VOF method; (iii) the unphysical motion of the interface can be avoided by using the buoyancy-modified k − ω SST model in long-time simulations. In addition, a new post-processing approach is proposed to evaluate the interface thickness. The decrease of interface thickness improves the accuracies of wave elevations by using the modified isoAdvector method. The adoption of both the modified isoAdvector method and the buoyancy-modified k − ω SST model improves the computational accuracies of wave elevations and hydrodynamic loads in long-time simulations.     

Homogenization of anisotropic elastoplastic behaviors of a porous polycrystal with interface effects

This paper is devoted to develop a theoretical framework to predict the macroscopic transversely isotropic elastoplastic behavior of clay‐like material, which is viewed as a porous polycrystal. We consider evolutions of two local plastic mechanisms of grains and interface simultaneously, for which a Schmid criterion is used for the strength of sheet‐like grains and a Tresca criterion for the strength of interfaces between particles. By adapting the standard incremental method, we propose firstly a classic self‐consistent model, which does not consider the effect of interface, then a generalized self‐consistent model in which the solid phase is represented by laminated (or isotropic) spherical grains surrounded by interfaces. Comparisons of numerical predictions between these two methods are performed and have demonstrated the validity of the generalized self‐consistent model taking account of interface effects. Numerical simulations of uniaxial compression tests have shown that the macroscopic elastoplastic behavior of polycrystalline (clay‐like) material can be successfully predicted by the way of considering the two local plastic mechanisms at microscopic scale. Copyright © 2013 John Wiley & Sons, Ltd.