Resolution of High-frequency Rayleigh-wave Data

2005 ◽  
Vol 10 (2) ◽  
pp. 99-110 ◽  
Author(s):  
J. Xia ◽  
C. Chen ◽  
G. Tian ◽  
R. D Miller ◽  
J. Ivanov
2007 ◽  
Author(s):  
Jianghai Xia ◽  
Richard D. Miller ◽  
Julian Ivanov

2000 ◽  
Vol 43 (3) ◽  
pp. 395-406 ◽  
Author(s):  
Guo-Ming XU ◽  
Guang-Pin LI ◽  
Shan-En WANG ◽  
Hong CHEN ◽  
Hu-Shun ZHOU
Keyword(s):  

2015 ◽  
Vol 771 ◽  
pp. 179-182 ◽  
Author(s):  
Yekti Widyaningrum ◽  
Sungkono ◽  
Alwi Husein ◽  
Bagus Jaya Santosa ◽  
Ayi S. Bahri

Rayleigh wave dispersion is intensively used to determine near surface of shear wave velocity (Vs). The method has been known as non-invasive techniques which is costly effective and efficient to characterize subsurface. Acquisition of the Rayleigh wave can be approached in two ways, i.e. passive and active. Passive seismic is accurate to estimate dispersion curve in low frequency, although it is not accurate for high frequency. While active seismic is vice versa of passive seismic. The high frequency of Rayleigh wave dispersion reflects to near surface and vice versa. Therefore, we used the combination of both passive and active seismic method to overcome the limitations of each method. The Vs which is resulted by inversion of the combining data gives accurate model if compared to log and standard penetration test (N-SPT) data. Further, the approach has been used to characterize LUSI (Lumpur Sidoarjo) embankments. The result shows that embankment material (0-12 m) has higher Vs than that lower embankment material.


2021 ◽  
Vol 64 (1) ◽  
Author(s):  
Xiang Min ◽  
Qi Xinghua ◽  
Zhang Fengwei

Rayleigh wave detection is a recently developed method for shallow seismic exploration. Current Rayleigh wave data processing and interpretation methods can only provide the transverse average wave velocity of rock-soil bodies under the geophone array range, resulting in a low lateral resolution of wave velocity. To solve this problem, this paper presents a Rayleigh wave data processing method based on wavelet transform. First, the Hankel matrix is constructed from the intercepted Rayleigh wave, and the effective singular value is preserved by singular value decomposition to filter the Rayleigh wave. Then, the appropriate center frequency is selected and the corresponding relationship between the time and frequency of the Rayleigh wave is obtained via wavelet transform. The waveform of each frequency component can be extracted and the complete time difference of each frequency component between two geophones will be obtained and used to calculate the phase velocity-depth profile of the Rayleigh wave in a rock-soil body. This method is applied to examine unfavorable geological bodies that are underground in a yard. By combining the phase velocity-depth profiles of several survey lines, the 3-D image of phase velocity of Rayleigh wave underground can be obtained. This method can provide the phase velocity distribution of the formation below the survey line by only one measurement, which greatly improves upon the work efficiency and lateral resolution of the traditional Rayleigh wave data processing method.


2015 ◽  
Vol 116 ◽  
pp. 93-103 ◽  
Author(s):  
Limin Wang ◽  
Yixian Xu ◽  
Jianghai Xia ◽  
Yinhe Luo

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