测震台网强震影响范围快速判定

以测震台网Jopens系统流服务为依托,根据NetSeis/IP协议通讯标准实时接收数据包,解析MiniSEED格式波形数据,监控台站波形中断情况,实现基于REST架构的台站状态显示,结合震中附近地质构造信息,快速判定地震破坏扩展方向,圈定极震区范围,为地震应急决策服务.     

Application of passive source surface-wave method in site engineering seismic survey

Site engineering seismic survey provides basic data for seismic effect analysis. As an important parameter of soil, shear-wave velocity is usually obtained through wave velocity testing in borehole. In this paper, the passive source surface-wave method is introduced into the site engineering seismic survey and practically applied in an engineering site of Shijingshan District. By recording the ubiquitous weak vibration on the earth surface, extract the dispersion curve from the surface-wave components using the SPAC method and obtain the shear-wave velocity structure from inversion. Over the depth of 42 m underground, it totally consists of five layers with interface depth of 3.31, 4.50, 7.23, 17.41, and 42.00 m; and shear-wave velocity of 144.0, 198.3, 339.4, 744.2, and 903.7 m/s, respectively. The inversion result is used to evaluate site classification, determine the maximum shear modulus of soil, provide basis for further seismic hazard analysis and site assessment or site zoning, etc. The result shows that the passive source surface-wave method is feasible in the site engineering seismic survey and can replace boreholes, shorten survey period, and reduce engineering cost to some extent.     

Mechanism on Moho offset induced by aseismic slip of deeply buried faults

Recent high-resolution deep seismic reflection profile across the Kunlun fault in northeastern Tibet shows clearly that the Moho is cut off by a complex thrust fault system. Moho offset is a general phenomenon, but little is known about the dynamic mechanism. In this study, contact models with Maxwell materials are used to simulate the mechanical process of Moho offset induced by the aseismic slip of deeply buried faults. Based on the seismic reflection data, we project a single fault model and a complex fault system model with two faults intersecting. The deformations of the Moho, the aseismic slips, and contact stresses on faults in different models are discussed in detail. Results show that the Moho offset might be produced by aseismic slip of deeply buried faults, and the magnitude is influenced by the friction coefficient of faults and the viscosity of the lower crust. The maximum slip occurs near the Moho on the single fault or at the crossing point of two intersecting faults system. Stress concentrates mainly on the Moho, the deep end of faults, or the crossing point. This study will throw light on understanding the mechanism of Moho offset and aseismic slip of deeply buried faults. The results of complex fault system with two faults intersecting are also useful to understand the shallow intersecting faults that may cause earthquakes.     

Aftershock sequence simulations using synthetic earthquakes and rate-state seismicity formulation

We use an efficient earthquake simulator that incorporates rate-state constitutive properties and uses boundary element method to discretize the fault surfaces, to generate the synthetic earthquakes in the fault system. Rate-and-state seismicity equation is subsequently employed to calculate the seismicity rate in a region of interest using the Coulomb stress transfer from the main shocks in the fault system. The Coulomb stress transfer is obtained by resolving the induced stresses due to the fault patch slips onto the optimal-oriented fault planes. The example results show that immediately after a main shock the aftershocks are concentrated in the vicinity of the rupture area due to positive stress transfers and then disperse away into the surrounding region toward the background rate distribution. The number of aftershocks near the rupture region is found to decay with time as Omori aftershock decay law predicts. The example results demonstrate that the rate-and-state fault system earthquake simulator and the seismicity equations based on the rate-state friction nucleation of earthquake are well posited to characterize the aftershock distribution in regional assessments of earthquake probabilities.     

Soil phosphorus bioavailability assessed by XANES and Hedley sequential fractionation technique in a glacier foreland chronosequence in Gongga Mountain,Southwestern China

The primary productivity of terrestrial ecosystems is influenced by soil phosphorus bioavailability, which depends largely on chemical fractions of phosphorus. The sequential fractionation technique developed by Hedley et al. or its subsequent modification is a well-known method to determine soil phosphorus forms. Hedley sequential fractionation technique separates the phosphorus into fractions based on their different chemical solubilities in extractants with certain chemical properties. Recently, synchrotron-based X-ray absorption near edge structure (XANES) spectroscopy has been employed to measure soil phosphorus species directly and non-invasively. The XANES method provides information concerning local structure and chemical information of target elements at a molecular level. Thus, it can distinguish phosphorus fractions bound by metal oxides or hydroxides (such as Fe, Al, and Ca). In this present work, the phosphorus speciation of topsoil along a glacial foreland chronosequence in Gongga Mountain is determined using these two methods. The changes in soil phosphorus bioavailability along the 120-year-old chronosequence are assessed based on comparisons of the results obtained by these two methods. The results indicate that Hedley sequential fractionation technique shows a greater ability to determine soil bioavailable phosphorus (Resin-P and NaCHO₃-P), while XANES is effective in distinguishing phosphorus bound by metal compounds. In the chronosequence, Ca- and Al-bound phosphorus were derived mainly from primary minerals, whose phosphorus contents decreased within 120 years of moraine weathering and soil development. The content of soil bioavailable phosphorus increased rapidly after 30 years since deglaciation. The increasing phosphorus bioavailability promoted the colonizing and primary succession vegetation.     

上边界条件对多年冻土地温场数值模拟结果的影响分析

以玛多地区多年冻土为背景,建立多年冻土地温场的数值计算模型,以不同的方式考虑近 60 a 来的气温变化构成不同的上边界条件,通过模型计算分析不同上边界条件下的不同时期温度场、未来冻土退化特征.结果表明：在上边界条件中采用气象站实测近60 a波动温度值和采用近60 a平均恒定值时,浅层冻土地温差异明显,且越浅层地温与越近时间的上边界条件相关.预测未来100 a冻土地温变化趋势发现,相同升温速率和升温初始温度条件下,上边界采用实测60 a波动温度值对冻土退化过程影响较小;升温初始温度值提高到与趋势线衔接后,冻土退化起始时间从约第45年提前到约第20年;60 a实测温度和升温初始温度值均提高到与其初始温度场上边界条件衔接后,冻土退化起始时间从约第20年提前到约第15年;冻土退化从开始到完全退化经历时间为25 a左右.     

青海省共和-玉树高速公路新建块石路基下的温度状况分析

块石路基是多年冻土区应用最为广泛的多年冻土路基形式. 为了研究多年冻土区修筑高速公路后块石路基的效果,选取青海省新建共和-玉树高速公路3个块石路基监测断面的实测资料,对路基修筑初期多年冻土温度状况进行了分析. 结果表明：路基修筑初期路基中心原天然地表下0.5 m处仍表现出季节变化规律,至原多年冻土上限深度处,温度波动幅度急剧减小. 块石路基的保温效果与年平均地温密切相关,年平均地温越低,对冻土的保护效果越显著. 受阴阳坡效应的影响,左路肩/坡脚温度高于右路肩/坡脚. 左右路肩及中心孔下多年冻土上限都得到不同程度的抬升,抬升幅度主要受路基高度影响,与多年冻土年平均地温没有必然关系.     

祁连山大通河源多年冻土区浅层土壤水热时空变化特征

在大通河源不同草甸生态系统中建立浅层土壤水热监测网络. 2010-2011年监测结果表明：土壤温度和水分均具有明显的冻融交替和空间梯度变化格局. 在沼泽化草甸和典型草甸区,土壤融化和冻结末期分别出现在5月底、6月初和11月中下旬;而退化草甸区对应的时间则出现在4月底、5月初和11月中上旬. 在沼泽化草甸和典型草甸土壤温度变化曲线上有明显的“零点幕”时期,而退化草甸则不太明显. 土壤温度曲线的阶段划分结果表明,沼泽化草甸和典型草甸各阶段不存在显著差异,二者阶段划分曲线基本重合,均可以划分为6个阶段：春季升温阶段、春季“零点幕”阶段、夏季升温阶段、秋季降温阶段、秋季“零点幕”阶段和冬季降温阶段. 对于退化草甸而言,春季和秋季“零点幕”时期不明显,阶段划分曲线与前二者具有较大差异. 退化草甸温度曲线“零点幕”时期不显著对应于下伏多年冻土临近岛状多年冻土边缘,是最易于受环境影响变化而发生退化的区域. 3个监测场地浅层土壤水热格局一定程度上指示了下伏多年冻土的空间分布格局.     

节理岩体超声测试及单轴压缩试验研究

为了获取节理岩体各向异性力学特性和声波传播规律的相互关系,通过制作圆柱形单一预制贯通节理试件,开展了7种不同倾角节理试件的超声波波速测试和单轴压缩试验。试验结果表明：（1）节理试件波速测试值离散性较大,但总体服从正态分布,波速平均值介于石膏试件和完整试件之间,波速随节理倾角增大呈线性递减;（2）不同倾角的节理面对节理试件力学特性的影响很大,在应力-应变关系、变形特征、强度特征和破坏模式上均表现出显著的各向异性特征;（3）节理试件的力学性质和超声波传播特性变化规律区别很大,采用超声波波速确定节理试件的力学参数会存在很大误差。     

南海琼东南盆地崖13-1气田古近系陵水组海陆过渡带沉积特征及演化*

南海北部琼东南盆地中的众多凹陷均有海陆过渡相沉积,沉积相类型包括海湾辫状河三角洲和河口湾-潮坪。本次研究以高分辨率层序地层学理论为指导,将崖13-1气田古近系渐新统陵水组三段及二段各划分为1个长期基准面旋回,并在其内部进一步识别出10个中期基准面旋回(S1-S10)。在等时地层格架内,对陵水组三段及陵水组二段发育的沉积相特征及演化进行深入的探讨。陵水组三段沉积时期,研究区主要发育海湾辫状河三角洲沉积,其具有独特的层理构造、富含泥质纹层以及遗迹化石丰富。该沉积体系自下而上潮汐作用越来越强,早期以河流作用为主(S1-S4),中期为河流和潮汐混合作用(S5-S6),晚期逐渐过渡到以潮汐作用占主导(S7-S8)。陵水组二段沉积时期,研究区发生全面海侵,沉积作用方式及沉积特征更加复杂,生物成因构造更加独特,本次研究将其解释为河口湾-潮坪沉积(S9-S10)。研究表明,区域海平面的不断上升是研究区沉积相从海湾辫状河三角洲演化到河口湾-潮坪的主要控制因素。