地震动输入界面的选取对深软场地地震效应的影响

以天津和上海两个典型的深厚软弱场地为研究背景,探讨了地震动输入界面对场地地表地震动参数的影响。对于场地1(天津)和场地2(上海),分别选择7个和8个剪切波速(υs)大小不同的土层位置作为地震动输入界面,并选用Taft、Northridge地震加速度记录和南京人工波作为输入地震动,将Taft波、Northridge波和南京人工波的加速度峰值水平调整为0．35m／s^2、0．70m／s^2和0．98m／s^2,用SHAKE91程序对这两个场地进行了不同的地震动输入界面、输入地震波和峰值加速度水平的128种组合的场地地震反应分析。与从假想基岩面(υs≥500m／s)输入地震动的结果(假想的实际值)相比,可得到如下结论：(1)随着地震动输入界面深度(剪切波速)的增加,场地地表加速度反应谱逐渐地向实际值接近;(2)地震动输入界面的深度相同时,地震动加速度峰值水平越高,两者的加速度反应谱谱值的相对差异也越大;(3)对于一般建筑物,可以把剪切波速为400m／s左右的土层作为地震动输入界面;对于中长周期的建筑物,则应慎重选择地震动输入界面,最好选取υs≥500m／s^2的土层或基岩面作为地震动输入界面。     

地震反应分析中输入界面的选取对地表地震动参数的影响

地震反应分析中输入界面选取合理与否对设计地震动参数有重要影响。基于唐山地区钻孔剖面,分别选取剪切波速为500m/s的硬黏土和800m/s的岩石顶面作为基岩输入界面,采用一维等效线性化方法讨论中硬场地输入界面的选取对地表地震动参数的影响,结果表明:(1)地表峰值加速度放大倍数及地表加速度反应谱特征周期都随输入界面深度的增加而递增,且这种递增与输入地震动的强度及频谱特性都有密切联系;(2)随着输入界面深度的增加,地表加速度反应谱几乎全频段内增大,仅在短周期内出现减小的情况,但幅度十分有限;(3)中硬场地地震反应分析中基岩输入界面宜取剪切波速为800m/s的土层顶面。     

控制性深孔地震输入界面位置的确定方法和影响研究

探讨了在工程场地地震安全性评价的地震反应分析模型中,江苏省盐城地区部分工程场地内深度超过100m时剪切波速仍小于500m/s的控制性深孔,采用近似估算方法弥补所缺波速值和确定地震输入界面后,进行波速值和地震输入界面位置的不确定性对工程场地地震反应的影响研究,包括地表地震动峰值加速度和反应谱特征周期等,为其他地区控制性深孔的地震输入界面位置的确定方法和影响研究提供参考。     

土层剪切波速测试中的不确定性对场地地震动参数的影响分析——以Ⅲ类场地为例

本文选取山东地区2个Ⅲ类场地的工程地质勘探及土层剪切波速等资料,将土层厚度按5个深度段,每个分段给出了4个土层剪切波速的改变量,通过改变不同深度段土层剪切波速,建立了19种土层地震反应分析模型,分析了不同深度段,不同概率水平下土层剪切波速的变化对场地地震动参数的影响。研究表明,不同深度段土层剪切波速的变化对场地地震动参数的影响有差异。具体表现为,土层剪切波速的改变在1—10m、11—40m和地震输入界面处三个深度段对地震动加速度峰值影响较大;其中,41—70m和71—100m两个深度段剪切波速的改变对地震动加速度峰值影响小;在土层深度1—10m时,剪切波速降低,峰值变大,剪切波速的改变与峰值的改变呈负相关;在其它深度段,剪切波速降低,峰值变小,剪切波速的改变与峰值的改变呈正相关。剪切波速的改变在1—10m和11—40m两个深度段对地震加速度反应谱影响较大;在41—70m、71—100m和地震输入界面三个深度段对地震加速度反应谱影响很小。     

输入界面对场地地表地震动参数的影响

本文以江淮地区典型场地资料为原型,选取不同深度的岩层位置作为地震动输入界面,构造多种场地土层模型,选择Taft、Kobe和E1centro 3条强震记录作为地震输入,采用一维频域等效线性化波动方法重点分析了地震动输入界面对场地地表地震动参数的影响。研究结果表明,随着输入界面深度的增加,场地地表的峰值加速度逐渐增加,且增加的幅度呈逐渐减小的趋势,但输入界面深度对地表加速度反应谱特征周期的影响较小;输入界面剪切波速值对反应谱特征周期影响有限,但对地表峰值加速度影响较为显著,地表峰值加速度随着输入界面剪切波速的增大而增大,且两者的增幅呈现近似的线性关系。     

含软弱夹层土深厚场地输入界面的确定

为研究含软弱夹层土深厚场地输入界面的确定方法,在一个场地剖面的基础上,另外构造了一个特殊场地剖面,计算了两个剖面在6个强度的地震动输入下,输入界面选择在不同位置时的峰值加速度A_(max),特征周期T_g和反应谱平台值α_(max),分析了两种土层剖面的地表地震动参数对输入界面改变的敏感性。结果发现特殊场地的敏感性较差,输入界面深度相差44.4m,剪切波速相差111m/s,但得到A_(max)、T_g和α_(max)相差不到10%、12%和8%,所以深厚的特殊场地在确定输入界面时,可以适当放宽对输入界面深度和剪切波速的要求,可满足一般工程的精度要求。     

场地条件对地表峰值加速度的放大效应分析

在研究西安地区大量钻孔资料的基础上,构造了44个不同等效剪切波速和覆盖层厚度场地条件下的典型场地剖面,利用一维等效线性化地震反应分析方法,计算了不同场地在3种不同强度的地震动输入下的地面峰值加速度,分析了地震动峰值加速度放大系数ks随场地类别、等效剪切波速Vse、覆盖层厚度H和输入地震动强度ar的变化特征,指出了按场地类别对地震动峰值加速度调整存在的问题。分析结果表明,加速度放大系数随等效剪切波速、覆盖层厚度及基岩输入地震动强度的增大而减小;等效剪切波速对加速度放大系数的影响大于覆盖层厚度的影响,随着输入地震动强度的增大,覆盖层厚度对加速度放大系数的影响成份有逐渐加大的趋势;覆盖层厚度对加速度放大系数的影响程度随着等效剪切波速的增大而逐渐减弱;加速度放大系数与场地等效剪切波速和覆盖层厚度之间具有较高的拟合度的统计回归关系。由此提出了直接用场地等效剪切波速和覆盖层厚度对地震动峰值加速度进行调整的新途径。最后,就地震动峰值加速度随场地条件的调整方法,提出了有待进一步研究的问题。     

地震动输入界面的选取对地震动参数的影响

地震反应分析中的输入界面是一种规定的假想基岩面,其选取具有很大的不确定性,对确定地震动参数的影响很大.本文以北京地区存在剪切波速较高的卵石硬夹层场地为研究对象,探讨实际工程场地中能否将硬夹层选作地震动输入界面的问题.利用一维等效线性化波动方法,对390个含有剪切波速高于500m/s的卵石层场地模型进行地震反应分析计算,讨论卵石层的上覆土层、下伏土层以及卵石层自身特性对地震反应分析结果的影响.计算结果显示,厚度5m左右、剪切波速小于600m/s的卵石层作为地震动输入界面是否合理,主要取决于上覆土层和下伏土层,而卵石层厚度和剪切波速的影响很小.对于一般性工程,当上覆土层厚度大于15m,下伏土层厚度在10m以内时,选取硬夹层顶面与选取钻探揭示的基岩或剪切波速不小于500m/s的土体顶面为输入界面,计算结果差别不大;当上覆土层厚度达到60m,下伏土层的变化对计算结果影响很小.研究表明,在钻探没有揭示出基岩或坚硬土体时,埋深大于60m的硬夹层可以选为地震动输入界面,这一结论对实际的地震安全性评价工作具有一定参考价值.     

Analysis of Influence Characteristics of Site Ground Motion in Ya'an Area,Sichuan

为分析雅安地区场地结构引起的震动特性,选取该地区重大安评项目中的实际测试钻孔进行场地地震反应分析,采用等效线性化方法,并以NGA强震记录为输入,开展场地反应计算,在全面分析该地区场地地震特征的基础上,以峰值速度为参数指标,研究场地条件引起的峰值速度放大效应。研究结果表明,雅安地区场地卓越周期约为0.2 s,自振周期为0.2 s的建筑结构破坏相对严重;随着基岩峰值加速度的增大,峰值速度呈增大趋势,峰值速度与峰值加速度变化趋势并非完全一致,分析场地效应时应考虑多种地震动参数的变化规律;不同地震输入下峰值速度放大系数为1～1.8;峰值速度放大系数k_v在不同强度基岩输入下,大致呈随等效剪切波速的增大而减小的趋势,软土场地更易引起场地峰值速度的放大,这种现象在芦山地震中较为明显。     

剪切波速对场地地表地震动参数的影响

本文以江淮地区典型场地资料为原型,将土层剪切波速实测值按照一定比例进行增减,构造多种场地土层地震反应分析模型,选择Taft、E1centro和Kobe三条强震记录作为地震输入,采用一维频域等效线性化波动方法进行了土层地震反应分析.研究结果表明,剪切波速的变异性与场地地表地震动的影响程度与输入基岩地震动的频谱特性、幅值、土层结构等因素有关.地表峰值加速度随着剪切波速的增大而逐渐增大,地表加速度反应谱的特征周期随着剪切波速的增大而逐渐减小.     

Comparison of Sesimic Body Wave and Coda Wave Measures of Q

—Measurements of seismic attenuation (Q ^?1) can vary considerably when made from different parts of seismograms or using different techniques, particularly at high frequencies. These discrepancies may be methodological, or may reflect earth processes. To investigate this problem, we compare body wave with coda Q ^?1 results utilizing three common techniques i) parametric fit to spectral decay, ii) coda normalization of S waves, and iii) coda amplitude decay with lapse time. Q ^?1 is measured from both body and coda waves beneath two mountain ranges and one platform, from recordings made at seismic arrays in the Caucasus and Kopet Dagh over paths ≤ 4° long. If Q is assumed frequency independent, spectral decay fits show Q _s and Q _coda near 700–800 for both mountain paths and near 2100–2200 for platform paths. Similar values are determined with the coda normalization technique. However, frequency-dependent parameterizations fit the data significantly better, with Q _s ?(1 Hz) and Q _coda?(1 Hz) near 200–300 for mountain paths and near 500–600 for platform paths. Lapse decay measurements are close to the frequency-dependent values, showing that both spectral and lapse decay methods can give similar results when Q has comparable parameterizations. Above 6 Hz, coda measurements suggest some enrichment relative to body waves, perhaps due to scattering, but intrinsic absorption appears to dominate at lower frequencies. All approaches show sharp path differences between the Eurasian platform and adjacent mountains, and all are capable of resolving spatial variations in Q.     

Shear Wave Velocity Structure of the Sinai Peninsula from Rayleigh Wave Analysis

The lithospheric structure of the Sinai Peninsula is shown by means of nine shear velocity profiles for depths ranging from zero to 50 km, determined from the Rayleigh wave analysis. The traces of 30 earthquakes, which occurred from 1992 to 1999 in and around the study area, have been used to obtain Rayleigh wave dispersion. These earthquakes were registered by a broadband station located in Egypt (KEG station). The dispersion curves were obtained for periods between 3 and 40 s, by digital filtering with a combination of MFT and TVF filtering techniques. After that, all seismic events were grouped in source zones to obtain a dispersion curve for each source-station path. These dispersion curves were inverted according to generalized inversion theory, to obtain shear wave velocity models for each source-station path, which is the main goal of this study. The shear velocity structure obtained for the Sinai Peninsula is shown through the shear velocity distributions with depth. These results agree well with the geology and other geophysical results, previously obtained from seismic and gravity data. The obtained velocity models suggest the existence of lateral and vertical heterogeneity. The shear velocity increases generally with depth for all paths analyzed in the study area. Nevertheless, in some paths a small low velocity channel in the upper or lower crust occurs. Along these profiles, it is found that the crustal structure of the Sinai Peninsula consists of three principal layers: upper crust with a sedimentary layer and lower crust. The upper crust has a sedimentary cover of 2 km thick with an average S-velocity of 2.53 km/s. This upper crust has a variable thickness ranging from 12 to 18 km, with S-wave velocity ranging from 3.24 to 3.69 km/s. The Moho discontinuity is located at a depth of 30 km, which is reflected by a sharp increase in the S-velocity values that jump from 3.70–4.12 to 4.33–4.61 km/s.     

Wave radiation stress

There are differences in the literature concerning the vertically dependent equations that couple currents and waves. In this paper, currents are purposely omitted until the end. Isolating waves from currents allows one to focus on two main topics: an explanation of Stokes drift with apparent mean vorticity obtained from an otherwise irrotational flow and the determination of vertically dependent wave radiation stress which, when vertically integrated, conforms to that obtained by Longuet-Higgins and Stewart (1964) and Phillips (1977) nearly 50 years ago and, more recently, by Smith (2006). Discussion begins with the simple case of nonlinear flow beneath a stationary wavy wall.     

Wave moment geodynamics

The work presents a review of natural-science representations on the rotary motion of matter and its piecewise structure. Development of dense GPS-networks allowed to experimentally confirm the concept of block structures of the geophysical environment and to prove rotary character of block movement. An analysis of both the migration of earthquake sources and the movement of sections of tectonic plates’ borders has allowed to reveal general properties of such movements and to prove their wave nature. It is shown that within the limits of rotational model, blocks and plates are interconnected among themselves by the elastic long-range fields forming a uniform planetary geodynamic field. It is offered to use the geodynamic solutions of rotational model in the one class of phenomena as a basis at the construction of a new geological paradigm — wave moment geodynamics.     

瑞雷波勘探的研究现状及展望

作为一种新兴的岩土工程地球物理勘探方法，瑞雷波勘探具有其它方法无法比拟的优点，国内外关于瑞雷波勘探方面的实践和理论研究目前日益增多。本文对国内外瑞雷波勘探方法研究进行了综述，从正演、频散曲线的求取、反演三个方面对瑞雷波勘探的研究现状进行了详细总结，并探讨了当前瑞雷波勘探中存在的实践和理论问题，展望了该方法的发展趋势。     

Prediction of the Shear Wave Velocity from Compressional Wave Velocity for Gachsaran Formation

Shear and compressional wave velocities, coupled with other petrophysical data, are very important for hydrocarbon reservoir characterization. In situ shear wave velocity (Vs) is measured by some sonic logging tools. Shear velocity coupled with compressional velocity is vitally important in determining geomechanical parameters, identifying the lithology, mud weight design, hydraulic fracturing, geophysical studies such as VSP, etc. In this paper, a correlation between compressional and shear wave velocity is obtained for Gachsaran formation in Maroon oil field. Real data were used to examine the accuracy of the prediction equation. Moreover, the genetic algorithm was used to obtain the optimal value for constants of the suggested equation. Furthermore, artificial neural network was used to inspect the reliability of this method. These investigations verify the notion that the suggested equation could be considered as an efficient, fast, and cost-effective method for predicting Vs from Vp.     

长周期形变波特征分析

利用一些大地震前观测到的短临和临震地震前兆异常资料,综述了多年来长周期形变波观测事实和研究状况.利用地震前后记录到的典型震例异常图像的特点、形态、量级,多层次分析了长周期形变波的异常持续时间,有效监测范围,主震震级范围,异常形态,周期及传播速度特性.结果表明:长周期形变波异常持续时间多为震前几个小时到6.5天,对应地震...     

大理岩的波速各向异性测量

利用 GC- 1 0 0型工程多波参数分析仪 ,对山东莱州大理岩进行了波速各向异性的实验室观测。实验采用两组岩样 ,一组为带有先天的优势定向排列裂缝的岩样 ,另一组为带有优势层理走向的完整岩石。在未加载的状态下 ,发现两组岩样都有明显的波速方位各向异性。对于带有先天的优势定向排列裂缝的岩样 ,甚至可以在无加载状态下观测到剪切波的分裂现象     

Tectonic Stress Wave,Microfracture Wave,and a Modified Elastic-Rebound Model of Earthquakes

Based on a sample of some real earthquakes,we have suggested in previous papers that there is a density-tectonic stress wave with ultra-low frequency which is emitted from the epicenter region for months before earthquakes,and a micro-fracture wave 1 ～ 10 days before earthquakes. The former has been observed by different kinds of measurements and the latter has been observed by a few chance observations which consists of electromagnetic,gravitational and sonic fluctuations. We show real observational results that depict the two waves and they have very different frequencies,which are not difficult to discriminate. The classical elastic-rebound model is one of the most influential theories on earthquakes,and the thermodynamic elastic-rebound model has amended the classical framework. Considering the two waves above,we attempt to further modify the elasticrebound model,and the new framework could be called the "micro-fracture elasticrebound model". We infer that tectonic earthquakes could have three special phases: the accumulation of tectonic stress,micro-fracture,and main-fracture. Accordingly,there would be three waves which come from the epicenter of a tectonic earthquake,i. e. ,the tectonic stress wave with ultra-low frequency a few months before the earthquake,the micro-fracture wave about 1 ～ 10 days before the earthquake and the main-fracture wave (common earthquake wave).     

高频GPS形变波与地震波在日本MW9.0地震中的对比研究

高频GPS动态监测可快速准实时解算地表位移,其在地震参数快速确定、地壳形变短期变化过程、震源破裂过程和震级标度研究等方面成为传统地震学的补充。针对浙江省内的1Hz的GPS数据,本文采用GAMIT的TRACK模块,获得了日本2011年3月11日M_W9.0地震的位移时间序列,并将其与浙江省地震台网并址观测的地震计获得的位移信号进行对比。结果显示,高频GPS与地震计获得的峰值地动位移之间差异在GPS的观测误差范围内。相对于原始波形,两者在0.005～0.1Hz频段上的水平方向相关系数提高了50%以上,高程方向相关系数提高了2倍以上。研究表明,高频GPS与宽频带地震计的观测结果在时序和频谱上有相互重合的区域,GPS和地震仪可以共同覆盖地震地表位移的全部可能范围。