The diffraction of Rayleigh waves by a fluid-saturated alluvial valley in a poroelastic half-space modeled by MFS

Two dimensional diffraction of Rayleigh waves by a fluid-saturated poroelastic alluvial valley of arbitrary shape in a poroelastic half-space is investigated using the method of fundamental solutions (MFS). To satisfy the free surface boundary conditions exactly, Green's functions of compressional (PI and PII) and shear (SV) wave sources buried in a fluid-saturated poroelastic half-space are adopted. Next, the procedure for solving the scattering wave field is presented. It is verified that the MFS is of excellent accuracy and numerical stability. Numerical results illustrate that the dynamic response strongly depends on such factors as the incident frequency, the porosity of alluvium, the boundary drainage condition, and the valley shape. There is a significant difference between the diffraction of Rayleigh waves for the saturated soil case and for the corresponding dry soil case. The wave focusing effect both on the displacement and pore pressure can be observed inside the alluvial valley and the amplification effect seems most obvious in the case of higher porosity and lower frequency. Additionally, special attention should also be paid to the concentration of pore pressure, which is closely related to the site liquefaction in earthquakes. The diffraction of Rayleigh waves by a saturated poroelastic alluvial valley in a poroelastic half-space is accurately solved by the method of fundamental solutions (MFS).The results of dynamic displacement and pore pressure are presented both in frequency and time domain for different incident frequencies, alluvium porosities and boundary drainage conditions.It is revealed that the wave focusing effect both on the displacement and pore pressure can be observed inside the alluvial valley and the amplification effect seems more obvious for higher porosity and lower frequency.

[1]  C. Glorieux,et al.  Laser-induced surface modes at an air-porous medium interface , 2003 .

[2]  H. Deresiewicz The effect of boundaries on wave propagation in a liquid-filled porous solid: IV. Surface waves in a half-space , 1962 .

[3]  Marijan Dravinski,et al.  Scattering of plane harmonic P, SV, and Rayleigh waves by dipping layers of arbitrary shape , 1987 .

[4]  M. Markov Low-frequency Stoneley wave propagation at the interface of two porous half-spaces , 2009 .

[5]  R. Skalak,et al.  On uniqueness in dynamic poroelasticity , 1963 .

[6]  D. Schmitt,et al.  Measurement of the speed and attenuation of the Biot slow wave using a large ultrasonic transmitter , 2009 .

[7]  Arthur Frankel,et al.  A three-dimensional simulation of seismic waves in the Santa Clara Valley, California, from a Loma Prieta aftershock , 1992 .

[8]  Francisco J. Sánchez-Sesma,et al.  Destructive strong ground motion in Mexico city: Source, path, and site effects during great 1985 Michoacán earthquake , 1989 .

[9]  J. Anderson Strong ground motion from the Michoacan, Mexico , 1986 .

[10]  J. T. Rice,et al.  The effect of boundaries on wave propagation in a liquid-filled porous solid: V. Transmission across a plane interface , 1964 .

[11]  Shechao Feng,et al.  High-frequency acoustic properties of a fluid/porous solid interface. I. New surface mode , 1983 .

[12]  Mihailo D. Trifunac,et al.  The reflection of plane waves in a poroelastic half-space saturated with inviscid fluid , 2005 .

[13]  Arnaud Mesgouez,et al.  Transient mechanical wave propagation in semi-infinite porous media using a finite element approach , 2005 .

[14]  Arvind H. Shah,et al.  Amplification of obliquely incident seismic waves by cylindrical alluvial valley of arbitrary cross-sectional shape. Part II. Incident SH and rayleigh waves , 1991 .

[15]  J. Xia,et al.  Viscoelastic representation of surface waves in patchy saturated poroelastic media , 2014 .

[16]  B. Albers,et al.  Modeling Acoustic Waves in Saturated Poroelastic Media , 2005 .

[17]  M. Biot MECHANICS OF DEFORMATION AND ACOUSTIC PROPAGATION IN POROUS MEDIA , 1962 .

[18]  P. Nagy Observation of a new surface mode on a fluid‐saturated permeable solid , 1992 .

[19]  M. Sharma Surface waves in a general anisotropic poroelastic solid half-space , 2004 .

[20]  K. Attenborough,et al.  Generation of modally pure acoustic surface waves in a tapered partially filled duct , 2004 .

[21]  Jianwen Liang,et al.  Diffraction of plane P waves around an alluvial valley in poroelastic half-space , 2010 .

[22]  Jian-Hua Wang,et al.  Scattering of plane wave by circular-arc alluvial valley in a poroelastic half-space , 2008 .

[23]  M. Sharma Propagation and attenuation of Rayleigh waves in a partially-saturated porous solid with impervious boundary , 2015 .

[24]  C. Glorieux,et al.  Combined particle motion and fluid pressure measurements of surface waves , 2011 .

[25]  Kojiro Irikura,et al.  Basin Structure Effects on Long-Period Strong Motions in the San Fernando Valley and the Los Angeles Basin from the 1994 Northridge Earthquake and an Aftershock , 1996 .

[26]  Y. Tsai,et al.  Strong Ground Motion Characteristics of the Chi-Chi, Taiwan Earthquake of September 21, 1999 , 2001 .

[27]  Love and Rayleigh waves in the San Fernando Valley , 1972 .

[28]  Keiiti Aki,et al.  A study on the response of a soft basin for incident S, P, and Rayleigh waves with special reference to the long duration observed in Mexico City , 1989 .

[29]  L. Weihua,et al.  Scattering of plane P waves by circular-arc alluvial valleys with saturated soil deposits , 2005 .

[30]  Jihong Ye,et al.  Strength failure of spatial reticulated structures under multi-support excitation , 2011 .

[31]  J G Anderson,et al.  Strong Ground Motion from the Michoacan, Mexico, Earthquake , 1986, Science.

[32]  B. Albers,et al.  Monochromatic surface waves on impermeable boundaries in two-component poroelastic media , 2005 .

[33]  M. Stern,et al.  Scattering of plane compressional waves by spherical inclusions in a poroelastic medium , 1993 .

[34]  V. W. Lee,et al.  Zero-stress, cylindrical wave functions around a circular underground tunnel in a flat, elastic half-space: Incident P-waves , 2010 .

[35]  W. Q. Chen,et al.  A mixture theory analysis for the surface-wave propagation in an unsaturated porous medium , 2011 .

[36]  K. Wilmanski,et al.  Asymptotic analysis of surface waves at vacuum/porous medium and liquid/porous medium interfaces , 2002 .

[37]  G. Drijkoningen,et al.  On wavemodes at the interface of a fluid and a fluid-saturated poroelastic solid. , 2010, The Journal of the Acoustical Society of America.

[38]  Yun-Min Chen,et al.  Scattering and refracting of plane strain wave by a cylindrical inclusion in fluid-saturated soils , 1998 .

[39]  Giuliano F. Panza,et al.  A hybrid method for the estimation of ground motion in sedimentary basins: Quantitative modeling for Mexico city , 1994 .

[40]  Zhanfang Liu,et al.  Dispersion and Attenuation of Surface Waves in a Fluid-Saturated Porous Medium , 1997 .

[41]  M. Schanz,et al.  Wave propagation in a simplified modelled poroelastic continuum: fundamental solutions and a time domain boundary element formulation , 2005 .

[42]  Andrew N. Norris,et al.  Stoneley-wave attenuation and dispersion in permeable formations , 1989 .

[43]  E. Glushkov,et al.  Influence of porosity on characteristics of rayleigh-type waves in multilayered half-space , 2011 .

[44]  Francisco J. Sánchez-Sesma,et al.  An indirect boundary element method applied to simulate the seismic response of alluvial valleys for incident P, S and Rayleigh waves , 1993 .

[45]  Chiang C. Mei,et al.  A boundary layer theory for Rayleigh Waves in a porous, fluid-filled half space , 1983 .

[46]  T. Shimogo Vibration Damping , 1994, Active and Passive Vibration Damping.

[47]  M. Stastna,et al.  Poroelastic acoustic wave trains excited by harmonic line tractions , 2008, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[48]  V. W. Lee,et al.  A Note on Response of Shallow Circular Valleys to Rayleigh Waves: Analytical Approach , 1990 .