Rayleigh wave and detection of low-velocity layers in a stratified half-space

被引:34
作者
Zhang, BX [1 ]
Lu, LY [1 ]
机构
[1] Chinese Acad Sci, Inst Acoust, Beijing 100080, Peoples R China
基金
中国国家自然科学基金;
关键词
D O I
10.1134/1.1608975
中图分类号
O42 [声学];
学科分类号
070206 ; 082403 ;
摘要
The excitation and propagation of the guided waves in a stratified half-space and a Rayleigh wave exploration method in shallow engineering seismic exploration are studied in this paper. All the modes of the guided waves are calculated by the bisection method in the case where the low velocity layers are contained in a stratified half-space. Cases when the formation shear wave velocity gradually decreases from the top to the bottom layers are also studied. The dispersion curves obtained in actual Rayleigh wave exploration are usually noncontinual zigzag curves, but the dispersion curves given by the elastic theory for given modes of the guided waves are smooth and continual curves. In this paper, the mechanism of zigzag dispersion curves in Rayleigh wave exploration is investigated and analyzed thoroughly. The zigzag dispersion curves can give not only the possible positions of the low-velocity layers but also the other information on the formation structure (fractures, oil, gas, etc.). It is found that the zigzag dispersion curves of the Rayleigh wave are the result of the leap of the modes and the existence of low velocity layers in a stratified half-space. The effects of the compressional wave velocity, shear wave velocity, and density of each layer on zigzag dispersion curves and the relationship of the low velocity layers to zigzag dispersion curves are also investigated in detail. Finally, the exploration depth of the Rayleigh wave is discussed. The exploration depth of the Rayleigh wave is equal to the wavelength multiplied by a coefficient that is variable and usually given by the work experience and the formation properties of the local work area. (C) 2003 MAIK "Nauka/Interperiodica".
引用
收藏
页码:516 / 528
页数:13
相关论文
共 24 条
[1]   DISPERSION FUNCTION COMPUTATIONS FOR UNLIMITED FREQUENCY VALUES [J].
ABOZENA, A .
GEOPHYSICAL JOURNAL OF THE ROYAL ASTRONOMICAL SOCIETY, 1979, 58 (01) :91-105
[2]  
BENMENAHEM A, 1968, B SEISMOL SOC AM, V58, P1519
[3]  
GUAN XP, 1993, CHINESE J GEOPHYS, V36, P96
[4]  
Harkrider D. G., 1964, B SEISMOL SOC AM, V54, P627
[5]  
Haskell N. A., 1953, B SEISMOL SOC AM, V43, P17, DOI DOI 10.1785/BSSA0430010017
[6]  
Huang J., 1991, GEOPHYSICAL GEOCHEMI, V15, P268
[7]  
LI YM, 1982, J GEOPHYS, V25, P131
[8]  
Malagnini L, 1997, B SEISMOL SOC AM, V87, P1413
[9]   ANALYSIS OF DISPERSIVE WAVES BY WAVE FIELD TRANSFORMATION [J].
MCMECHAN, GA ;
YEDLIN, MJ .
GEOPHYSICS, 1981, 46 (06) :869-874
[10]   DISPERSION FUNCTION COMPUTATIONS FOR UNLIMITED FREQUENCY VALUES - COMMENT [J].
MENKE, W .
GEOPHYSICAL JOURNAL OF THE ROYAL ASTRONOMICAL SOCIETY, 1979, 59 (02) :315-323