共查询到20条相似文献，搜索用时 15 毫秒
1.
目前完全弹性介质中面波频散特征的研究已较为完善,多道面波分析技术(MASW)在近地表勘探领域也取得了较好的效果,但黏弹介质中面波的频散特征研究依然较少.本文基于解析函数零点求解技术,给出了完全弹性、常Q黏弹和Kelvin-Voigt黏弹层状介质中勒夫波频散特征方程的统一求解方法.对于每个待计算频率,首先根据传递矩阵理论得到勒夫波复频散函数及其偏导的解析递推式,然后在复相速度平面上利用矩形围道积分和牛顿恒等式将勒夫波频散特征复数方程的求根问题转化为等价的连带多项式求解问题,最后通过求解该连带多项式的零点得到多模式勒夫波频散曲线与衰减系数曲线.总结了地层速度随深度递增和夹低速层条件下勒夫波频散特征根在复相速度平面上的运动规律和差异.证明了频散曲线交叉现象在复相速度平面上表现为:随频率增加,某个模式特征根的移动轨迹跨越了另一个模式特征根所在的圆,并给出了这个圆的解析表达式.研究还表明,常Q黏弹地层中的基阶模式勒夫波衰减程度随频率近似线性增加,而Kelvin-Voigt黏弹地层中的基阶模式勒夫波衰减程度随频率近似指数增加,且所有模式总体衰减程度强于常Q黏弹地层中的情况. 相似文献
2.
槽波地震勘探利用槽波的频散特性反演煤层的结构特征,故理论频散曲线的计算是一个重要方面.使用水平层状模型假设下的面波频散曲线计算方法能够计算煤层厚度恒定模型地震槽波频散曲线;但当煤层厚度变化时该方法不再适用.基于前人水平层状均匀介质模型的面波理论频散曲线计算方法,对于含煤三层模型,本文发展了煤层厚度变化情况下的地震槽波理论频散曲线计算方法,并使用该方法计算分析了不同厚度函数模型的频散曲线形态特征.研究表明：与稳定厚度煤层相比,煤层厚度变化使得地震槽波群速度成为与频率及传播射线在水平面投影路径相关的二元函数;射线路径上煤层厚度的变化使得频散曲线在群速度方向上压缩,群速度变化范围变小,且使处于最小值位置的埃里相群速度增大;而煤层厚度的线性变化模型频散曲线只与射线首、尾处的煤层厚度有关,与煤层厚度恒定模型相比,曲线形态不发生改变;煤层厚度呈非线性变化时,频散曲线形态上可能发生改变. 相似文献
3.
It has been known for many years that dispersivities increase with solute displacement distance in a subsurface. The increase of dispersivities with solute travel distance results from significant variation in hydraulic properties of porous media and was identified in the literature as scale‐dependent dispersion. In this study, Laplace‐transformed analytical solutions to advection‐dispersion equations in cylindrical coordinates are derived for interpreting a divergent flow tracer test with a constant dispersivity and with a linear scale‐dependent dispersivity. Breakthrough curves obtained using the scale‐dependent dispersivity model are compared to breakthrough curves obtained from the constant dispersivity model to illustrate the salient features of scale‐dependent dispersion in a divergent flow tracer test. The analytical results reveal that the breakthrough curves at the specific location for the constant dispersivity model can produce the same shape as those from the scale‐dependent dispersivity model. This correspondence in curve shape between these two models occurs when the local dispersivity at an observation well in the scale‐dependent dispersivity model is 1·3 times greater than the constant dispersivity in the constant dispersivity model. To confirm this finding, a set of previously reported data is interpreted using both the scale‐dependent dispersivity model and the constant dispersivity model to distinguish the differences in scale dependence of estimated dispersivity from these two models. The analytical result reveals that previously reported dispersivity/distance ratios from the constant dispersivity model should be revised by multiplying these values by a factor of 1·3 for the scale‐dependent dispersion model if the dispersion process is more accurately characterized by scale‐dependent dispersion. Copyright © 2007 John Wiley & Sons, Ltd. 相似文献
4.
Reduction of ground vibration by means of barriers or soil improvement along a railway track 总被引：3，自引：0，他引：3
Trains running in built-up areas are a source to ground-borne noise. A careful design of the track may be one way of minimizing the vibrations in the surroundings. For example, open or infilled trenches may be constructed along the track, or the soil underneath the track may be improved. In this work, the influence of the track design and properties on the level of ground vibration due to a vehicle moving with subsonic speed is examined. A coupled finite element-boundary element model of the track and subsoil is employed, adopting a formulation in the moving frame of reference following the vehicle. The computations are carried out in the frequency domain for various combinations of the vehicle speed and the excitation frequency. The analyses indicate that open trenches are more efficient than infilled trenches or soil stiffening–even at low frequencies. However, the direction of the load is of paramount importance. For example, the response outside a shallow open trench may change dramatically when horizontal load is applied instead of vertical load. 相似文献
5.
The dynamic response of a tunnel buried in a two-dimensional poroelastic soil layer subjected to a moving point load was investigated theoretically. The tunnel was simplified as an infinite long Euler–Bernoulli beam, which was placed parallel to the traction-free ground surface. The saturated layer was governed by Biot’s theory. Combined with the specified boundary conditions along the beam and saturated poroelastic layer, the coupled equations of the system were solved analytically in the frequency–wavenumber domain based on Fourier transform. The time domain responses were obtained by the fast inverse Fourier transform. The critical velocity of the considered structure was determined from the dispersion curves. The different dynamic characteristics of the elastic soil medium and the saturated poroelastic medium subjected to the underground moving load were investigated. It is concluded that, for coarse materials or fine materials subjected to the high-velocity loading, models ignoring the coupling effects between the pore fluid and the soil skeleton may cause errors. The shear modulus and the permeability coefficients of the saturated soil as well as the load moving velocity had significant influence on the displacement and pore pressure responses. 相似文献
6.
对套管井偶极弯曲模式波的频散特性进行了系统的数值考察、实例对比和分析.发现套管井弯曲波频散曲线随地层横波速度的降低,特别是地层横波速度小于2000 m·s-1以下,会迅速移向高频区,偶极弯曲波基础模式主频散区（或截止频率）可出现在13 kHz以上,以致超出了现行低频偶极子声波测井仪的激发与接收频带,这是一过去没有被研究者注意到的现象,并进一步被现场实例所证实.研究表明控制套管井弯曲波频散曲线主频散区位置的主要是钢套管的厚度和地层横波速度.对地层横波速度大于井孔流体声速的快速地层,在钢套管壁厚一定（8 mm）的情况下,频散曲线主频散区可移至11 kHz以上,可能出现的最大可能频域位置是同一井孔内径,井外全钢时的频散曲线上等于、小于地层横波速度那一段,这对各种地层和套管参数都是适用的.对地层横波速度小于等于井孔流体声速（1500 m·s-1）的慢速地层,弯曲波频散曲线随地层横波速度的降低移向高频区的特点更为明显,可能移至16 kHz以上;而套管厚度的影响,也比快速地层大的多,对地层横波速度小于1380 m·s-1的慢速地层,无论用多高的频率激发,都不能在现行使用的各类套管井（壁厚6~12 mm）中用偶极声波测井仪测到弯曲模式波. 相似文献
7.
8.
Caveats in Multi-modal Inversion of Seismic Surface Wavefields 总被引：1，自引：0，他引：1
We consider several examples demonstrating that the formal modal representation of surface wavefields often does not describe
adequately observable wave parameters, such as the phase and group velocity dispersion of higher modes. The main reason for
this is the existence in the medium of several waveguides or weakly coupled wavefields in the same waveguide. In such cases
the separation of neighboring higher modes may be impossible, and observed dispersion curves may significantly differ from
the ones predicted by the theory. From the example related to the studies of the crustal and upper mantle structure we found
that the difficulty in the separation of first and second crustal higher modes can be overcome by applying a special inversion
procedure. This procedure ignores the existence of a low velocity layer in the upper mantle when fitting the observable higher-mode
dispersion curve to the one predicted by the model. 相似文献
9.
A comprehensive study is performed on the dynamic behavior of offshore wind turbine (OWT) structure supported on monopile foundation in clay. The system is modeled using a beam on nonlinear Winkler foundation model. Soil resistance is modeled using American Petroleum Institute based cyclic p–y and t–z curves. Dynamic analysis is carried out in time domain using finite element method considering wind and wave loads. Several parameters, such as soil–monopile–tower interaction, rotor and wave frequencies, wind and wave loading parameters, and length, diameter and thickness of monopile affecting the dynamic characteristics of OWT system and the responses are investigated. The study shows soil–monopile–tower interaction increases response of tower and monopile. Soil nonlinearity increases the system response at higher wind speed. Rotor frequency is found to have dominant role than blade passing frequency and wave frequency. Magnitude of wave load is important for design rather than resonance from wave frequency. 相似文献
10.
This study presents a novel mathematical model for analysis of non-axisymmetrical solute transport in a radially convergent flow field with scale-dependent dispersion. A two-dimensional, scale-dependent advection–dispersion equation in cylindrical coordinates is derived based on assuming that the longitudinal and transverse dispersivities increase linearly with the distance of the solute transported from its injected source. The Laplace transform finite difference technique is applied to solve the two-dimensional, scale-dependent advection–dispersion equation with variable-dependent coefficients. Concentration contours for different times, breakthrough curves of average concentration over concentric circles with a fixed radial distance, and breakthrough curves of concentration at a fixed observation point obtained using the scale-dependent dispersivity model are compared with those from the constant dispersivity model. The salient features of scale-dependent dispersion are illustrated during the non-axisymmetrical transport from the injection well into extraction well in a convergent flow field. Numerical tests show that the scale-dependent dispersivity model predicts smaller spreading than the constant-dispersivity model near the source. The results also show that the constant dispersivity model can produce breakthrough curves of averaged concentration over concentric circles with the same shape as those from the proposed scale-dependent dispersivity model at observation point near the extraction well. Far from the extracting well, the two models predict concentration contours with significantly different shapes. The breakthrough curves at observation point near the injection well from constant dispersivity model always produce lesser overall transverse dispersion than those from scale-dependent dispersivity model. Erroneous dimensionless transverse/longitudinal dispersivity ratio may result from parametric techniques which assume a constant dispersivity if the dispersion process is characterized by a distance-dependent dispersivity relationship. A curve-fitting method with an example is proposed to evaluate longitudinal and transverse scale-proportional factors of a field with scale-dependent dispersion. 相似文献
11.
频率-贝塞尔变换方法(Frequency-Bessel Transform method,简称F-J方法)是一种分析微动信号的新方法,由于该方法采用频率矢量波数变换处理水平层状各向同性弹性模型中时空平稳随机分布的微动信号,所以从理论上可以提取出清晰的瑞利波基阶和高阶模态频散曲线,但是目前还没有相关的野外实验对此进行研究和应用.本文首先采用该方法对上海市苏州河地区采集的城市微动信号进行处理获得了频率-相速度谱,然后提取了多模态瑞利波频散曲线,最后通过粒子群算法对频散曲线进行联合反演,得到了浅地表0~70 m深度范围的S波速度结构,并且利用钻孔数据对反演的速度结构进行了验证.另外,本文还通过对比F-J方法和传统的SPAC(SPatial AutoCorrelation method)方法分别提取的频散曲线,展示了F-J方法在处理城市微动信号方面的优势.本文研究结果表明:(1)F-J方法可以从少量台站(21个台站)短时记录(1小时)的微动信号垂直分量中提取出清晰的基阶和高阶模态瑞利波频散曲线;(2)F-J方法提取的高阶模态频散曲线比传统SPAC方法提取的更加清晰,高频部分(>13 Hz)优势更为明显;(3)联合基阶和高阶模态频散曲线反演的浅地表速度结构更加精确,可以分辨出第四系沉积层中物性相差较小的速度界面和低速异常,在城市浅地表精细结构成像方面具有较好的应用前景. 相似文献
12.
利用在大形变基础上叠加小扰动的非线性波动理论——声弹性理论，数值考察了井外均匀各向同性固体介质同时受井孔静压力和井外单轴水平压力作用时，Stoneley波和两种偏振的偶极弯曲波的相速度频散曲线，并研究了计算中用到的灵敏系数随频率的变化. 数值结果表明，模式波相速度频散曲线的变化主要受灵敏系数中对应的3个三阶弹性常数的项控制；由井孔周围应力集中引起的沿单轴压力方向和垂直于该方向偏振的弯曲波发生分裂，同时随频率的增大，两条频散曲线产生交叉；井孔静压力的作用使两条频散曲线交叉点的位置发生变化，交叉点相速度值随井孔压力的增加而增大，但对应的频率值不变. 相似文献
13.
Rayleigh波可以用来反演近地表结构,在工程物探、石油物探、地球内部结构探测中均有重要意义.数值计算得到的含低速层的层状介质对应的Rayleigh波频散曲线会出现看似“交叉”的现象,但是对于这种现象目前还没有进行系统的研究.事实上可以验证,有些看似交叉的频散曲线实际上不相交.改变低速层的厚度和横波速度发现低速层越明显（即低速层速度越低或层厚越厚）频散曲线越不容易相交.凡友华等在2007年提出频散曲线对应着四种基本模式,在频散曲线发生“交叉”现象的区域实际上存在两个以上模式的频散曲线.本文主要研究了存在R模和S2模的区域内频散曲线的“交叉”现象.首先利用竖直本征振动曲线研究R模和S2模Rayleigh 波的振动特点,发现R模对应的本征振动主要集中在地表,随着深度变化能量快速衰减,S2模对应的本征振动主要集中在第2层.研究“交叉点”附近频散点对应的本征振动曲线发现这一区域有些Rayleigh波同时具有R模和S2模的振动特点,对应着一种耦合模式.通过对实例的研究发现,在“交叉点”附近,若两条频散曲线不发生交叉,则每条曲线对应的模式会发生R模和S2模之间经由耦合模式的转变,本文称这种现象为两种模式发生耦合;若两条频散曲线相交,则同一条频散曲线上的Rayleigh波模式几乎相同,只是在离交点很近的区域会存在一些耦合模式,本文称此时两种模式不发生耦合.本文研究结果主要供Rayleigh波对低速层结构的反演研究参考. 相似文献
14.
在研究轨道振动荷载的产生机理基础上,归纳出一个能够涵盖速度、线路不平顺、轮重、轨枕对轮载的分散作用等因素在内的轨道荷载解析表达式,以此作为输入施加到土体模型上,利用ANSYS模拟地基土在轨道移动荷载作用下的三维瞬态弹塑性反应。通过计算得到土体不同位置位移和加速度时程曲线,并得出如下结论:荷载刚施加时地面位移会有一个突变,但是随着荷载的移动会达到一个稳定值,并随着水平面内远离轨道,该值逐渐衰减;荷载刚刚施加时加速度会有一个突变值,随着荷载的移动逐渐趋于零。轨道机车速度对竖向方向的位移和加速度影响不大。 相似文献
15.
We present an analytical expression for the shear dispersion during solute transport in a coupled fracture–matrix system. The dispersion coefficient is obtained in a fracture with porous walls by taking into account an accurate boundary condition at the interface between the matrix and fracture, and the results were compared with those in a non-coupled system. The analysis presented identifies three regimes: diffusion-dominated, transition, and advection-dominated. The results showed that it is important to consider the exchange of solute between the fracture and matrix in development of the shear dispersion coefficient for the transition and advection-dominated regimes. The new dispersion coefficient is obtained by imposing the continuity of concentrations and mass fluxes along the porous walls. The resulting equivalent transport equation revealed that the effective velocity in a fracture increases while the dispersion coefficient decreases due to mass transfer between the matrix and fracture. A larger effective advection term leads to greater storage of mass in the matrix as compared with the classical double-porosity model with a non-coupled dispersion coefficient. The findings of this study can be used for modeling of tracer tests as well as fate, transport, and remediation of groundwater contaminants in fractured rocks. 相似文献
16.
Marc Wathelet Denis Jongmans Matthias Ohrnberger Sylvette Bonnefoy-Claudet 《Journal of Seismology》2008,12(1):1-19
Valuable information about one-dimensional soil structures can be obtained by recording ambient vibrations at the surface,
in which the energy contribution of surface waves predominates over the one of other types of waves. The dispersion characteristics
of surface waves allow the retrieval of the shear-wave velocity as a function of depth. Microtremor studies are usually divided
in two stages: deriving the dispersion (or auto-correlation) curve from the recorded signals and inverting it to obtain the
site velocity profile. The possibility to determine the dispersion curve over the adequate frequency range at one site depends
on the array aperture and on the wavefield spectra amplitude that can be altered by filtering effects due to the ground structure.
Microtremors are usually recorded with several arrays of various apertures to get the spectral curves over a wide frequency
band, and different methods also exist for processing the raw signals. With the objective of defining a strategy to achieve
reliable results for microtremor on a shallow structure, we analyse synthetic ambient vibrations (vertical component) simulated
with 333 broadband sources for a 25-m deep soil layer overlying a bedrock. The first part of our study is focused on the determination
of the reliable frequency range of the spectral curves (dispersion or auto-correlation) for a given array geometry. We find
that the wavenumber limits deduced from the theoretical array re sponse are good estimates of the valid spectral curve range.
In the second part, the spectral curves are calculated with the three most popular noise-processing techniques (frequency–wavenumber,
high-resolution frequency–wavenumber and spa tial auto-correlation methods) and inverted indi vidually in each case. The inversions are
performed with a tool based on the neighbour hood algorithm that offers a better estimation of the global uncertainties than
classical linearised methods, especially if the solution is not unique. Several array apertures are necessary to construct
the dispersion (auto-correlation) curves in the appropriate frequency range. Considering the final velocity profiles, the
three tested methods are almost equivalent, and no significant advantage was found for one particular method. With the chosen
model, all methods exhibit a penetration limited to the bedrock depth, as a consequence of the filtering effect of the ground
structure on the vertical component, which was observed in numerous shallow sites. 相似文献
17.
对于在Rayleigh波勘探中经常提取到的多模式频散曲线，如何在理论上对其特征进行描述是一个很有意义的问题. 本文根据Rayeigh波频散方程中传递矩阵具有的高频近似特征，提出了传递矩阵的高频近似分解公式，据此导出了频散方程的高频近似分解公式，并在此基础上，定义了Rayleigh波的4种基本模式(R模、S模、R型周期模和S型周期模). 根据频散方程具有的周期性特征，给出了周期模频散曲线之间的平均间隔近似公式，以及在任意频率和相速度段内频散方程根的数目（即多模式的激发数目）的预测公式. 在这些结果的基础上，本文最后提出了频散方程数值搜根的一种新方法. 相似文献
18.
Fabrice Hollender Cécile Cornou Aline Dechamp Kaveh Oghalaei Florence Renalier Emeline Maufroy Clément Burnouf Sylvette Thomassin Marc Wathelet Pierre-Yves Bard Vincent Boutin Clément Desbordes Isabelle Douste-Bacqué Laetitia Foundotos Cédric Guyonnet-Benaize Vincent Perron Julie Régnier Agathe Roullé Mickael Langlais Deborah Sicilia 《Bulletin of Earthquake Engineering》2018,16(6):2337-2365
Data provided by accelerometric networks are important for seismic hazard assessment. The correct use of accelerometric signals is conditioned by the station site metadata quality (i.e., soil class, VS30, velocity profiles, and other relevant information that can help to quantify site effects). In France, the permanent accelerometric network consists of about 150 stations. Thirty-three of these stations in the southern half of France have been characterized, using surface-wave-based methods that allow derivation of velocity profiles from dispersion curves of surface waves. The computation of dispersion curves and their subsequent inversion in terms of shear-wave velocity profiles has allowed estimation of VS30 values and designation of soil classes, which include the corresponding uncertainties. From a methodological point of view, this survey leads to the following recommendations: (1) perform both active (multi-analysis surface waves) and passive (ambient vibration arrays) measurements to derive dispersion curves in a broadband frequency range; (2) perform active acquisitions for both vertical (Rayleigh wave) and horizontal (Love wave) polarities. Even when the logistic contexts are sometimes difficult, the use of surface-wave-based methods is suitable for station-site characterization, even on rock sites. In comparison with previous studies that have mainly estimated VS30 indirectly, the new values here are globally lower, but the EC8-A class sites remain numerous. However, even on rock sites, high frequency amplifications may affect accelerometric records, due to the shallow relatively softer layers. 相似文献
19.
为了对比天然源面波勘探不同台阵布局的探测效果, 筛选出探测成果可靠、 效率高和便于野外施工的天然源面波勘探台阵阵形, 在天水市黄土覆盖区的同一场地分别用4种常见的阵形进行数据采集试验, 并对各种阵形数据使用空间自相关法或扩展空间自相关法提取相应的频散曲线, 通过反演得到了试验点地下的浅层速度结构模型. 分析对比试验结果表明: 4种台阵提取的频散曲线数值很相近; 频散谱能量集中度较高的是嵌套式等边三角形和圆形台阵, L形和直线形台阵相对分散; L形台阵低频段(4—8 Hz)比直线形台阵差, 其高频段(8—40 Hz)比直线形台阵好. 针对直线形台阵在高频段信噪比较低的情况, 在确保探测成果可靠性的前提下, 为了提高探测效率, 提出了在同一直线形台阵开展天然源与人工源面波联合勘探的数据采集方法. 实验结果证实, 这种联合勘探方法不仅可弥补直线形台阵高频段的不足, 确保探测精度和结果的可靠性, 而且还能实现“高低”频兼顾, 即“深浅”兼顾. 相似文献