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Study of surface wave methods for deep shear wave velocity profiling applied in the upper Mississippi embayment.

机译:密西西比河上游上游深层剪切波速度剖面的面波方法研究。

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摘要

Surface wave methods have become an important tool for non-intrusively and inexpensively determining shear wave velocity (Vs) profiles for many geotechnical earthquake engineering applications. The primary objectives of this study are to (1) compare active-source and passive (ambient vibration) surface wave methods for developing Vs profiles to depths of 200 to 300 m at deep soil sites, and (2) identify the primary factors affecting the reliability and consistency of surface wave methods. This comparative study became possible with the advent of a unique low-frequency field vibrator developed as part of the National Science Foundation's (NSF) Network for Earthquake Engineering Simulation (NEES) program. This vibrator is able to actively excite surface wave energy down to frequencies of less than 1 Hz. Four surface wave methods (two active-source methods and two passive-source methods) were applied in this study, namely: (1) the Spectral-Analysis-of-Surface-Waves (SASW) method, (2) the active-source frequency-wavenumber (f-k) method, (3) the passive-source frequency-wavenumber (f-k) method and (4) the refraction microtremor (ReMi) method. The focus of this study is on two critical aspects of surface wave methods: (1) development of a reliable surface wave dispersion curve from field measurements, and (2) compatibility between the experimental dispersion curve and the theoretical model used in the inversion procedure to develop the final Vs profile. Measurements were performed at eleven sites distributed over a distance of about 180 km in the upper Mississippi Embayment in the central United States, where soil deposits are hundreds of meters deep.;Limitations associated with each of the four methods were identified in this study. With respect to the SASW method it was found that potential phase unwrapping problems could cause an erroneous estimate of the dispersion curve. These errors were found to be associated with an abrupt mode transition caused by a strong velocity contrast at a shallow depth. With respect to the active-source f-k approach, it was demonstrated that near-field effects caused by a short near-source offset produced an underprediction of the surface wave dispersion curve at long wavelengths. Recommendations for acceptable source offset distances were developed based on the results from this study. The performance of the passive approaches (passive f-k method and ReMi method) was shown to be strongly dependent on the local ambient wavefield characteristics. Results from a study of the ambient wavefield characteristics at the 11 sites showed high ambient vibration levels at all sites in the frequency range of 1 to 4 Hz. Passive measurements using a circular array provided good comparisons with the active-source methods out to wavelengths of 500 m (2.5 times the array aperture) in most cases. Poor performance at one site was shown to be due to a multi-source wavefield at low frequencies. An improved comparison at this site was achieved by applying high-resolution processing methods. The ReMi method was found to provide good results down to frequencies of 3 to 4 Hz (wavelengths of 100 to 150 m) but very poor performance at lower frequencies ( 3 Hz). The wavefield characteristics at low frequencies were identified as the primary factor affecting the performance of the ReMi method.;Lastly, deep Vs profiles developed from active-source f-k dispersion curves using a fundamental mode inversion were compared with Vs profiles developed from SASW dispersion curves using an "effective-velocity" inversion. Good agreement between two inversion approaches was shown at most sites, however, large inconsistencies at depth were observed at one site. This inconsistency was shown to be due to incompatibility between the experimental dispersion curve and the fundamental mode model used in the inversion. The local site conditions, specifically the shallow depth of the Memphis Sand formation at this site was identified as the cause of the model incompatibility. Base on the findings from this study, recommendations for procedures to perform deep Vs profiling using surface waves are presented.
机译:对于许多岩土地震工程应用而言,表面波方法已成为一种重要的工具,可用于非侵入式且廉价地确定剪切波速度(Vs)剖面。这项研究的主要目的是(1)比较用于在深土层中将Vs剖面扩展到200至300 m深度的主动源和被动(环境振动)面波方法,以及(2)找出影响噪声的主要因素。面波方法的可靠性和一致性。随着作为国家科学基金会(NSF)地震工程仿真(NEES)计划网络开发的独特低频场振动器的出现,这项比较研究成为可能。该振动器能够主动激发低至1 Hz以下频率的表面波能量。本研究采用了四种表面波方法(两种有源方法和两种无源方法),即:(1)表面波频谱分析法(SASW),(2)有源源法。频率波数(fk)方法,(3)被动源频率波数(fk)方法和(4)折射微震(ReMi)方法。这项研究的重点是表面波方法的两个关键方面:(1)通过现场测量得出可靠的表面波色散曲线,(2)实验色散曲线与用于反演过程的理论模型之间的兼容性。制定最终的Vs档案。在美国中部密西西比河上游上部分布约180 km的11个地点进行了测量,那里的土壤沉积物深达几百米。这项研究确定了与这四种方法相关的局限性。关于SASW方法,发现潜在的相位解缠问题可能导致色散曲线的错误估计。发现这些错误与在浅深度的强速度对比引起的突然模式转变有关。关于有源光源f-k方法,已证明由短近源偏移引起的近场效应会导致对长波长表面波色散曲线的预测不足。根据这项研究的结果,提出了可接受的光源偏移距离的建议。被动方法(被动f-k方法和ReMi方法)的性能显示出强烈依赖于本地环境波场特性。对11个站点的环境波场特性进行研究的结果表明,所有站点在1到4 Hz频率范围内的环境振动水平都很高。在大多数情况下,使用圆形阵列的无源测量与有源光源方法在波长为500 m(阵列孔径的2.5倍)时可以很好地进行比较。结果表明,一个站点的性能较差是由于低频处的多源波场引起的。通过使用高分辨率处理方法,可以在此站点实现更好的比较。发现ReMi方法在3至4 Hz的频率(100至150 m的波长)下可提供良好的结果,但在较低的频率(<3 Hz)下性能却很差。低频波场特性被认为是影响ReMi方法性能的主要因素。最后,将使用基本模式反演的有源源fk色散曲线形成的深Vs曲线与使用SASW色散曲线形成的Vs曲线进行了比较。 “有效速度”反演。在大多数站点上,两种反演方法之间显示出良好的一致性,但是,在一个站点上,在深度上存在很大的不一致。结果表明,这种不一致是由于实验色散曲线与反演中使用的基本模式模型之间不兼容所致。当地的现场条件,特别是在该位置的孟菲斯沙层的浅层深度,被确定为模型不兼容的原因。根据这项研究的结果,提出了使用表面波进行深Vs剖面分析的程序的建议。

著录项

  • 作者

    Li, Jianhua.;

  • 作者单位

    University of Missouri - Columbia.;

  • 授予单位 University of Missouri - Columbia.;
  • 学科 Engineering Civil.
  • 学位 Ph.D.
  • 年度 2008
  • 页码 245 p.
  • 总页数 245
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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