Wave propagation characteristics in porous medium containing a solid in pores

被引:1
作者
Liu Lin [1 ,2 ,3 ]
Zhang Xiu-Mei [1 ,2 ,3 ]
Wang Xiu-Ming [1 ,2 ,3 ]
机构
[1] Chinese Acad Sci, Inst Acoust, State Key Lab Acoust, Beijing 100190, Peoples R China
[2] Univ Chinese Acad Sci, Beijing 100149, Peoples R China
[3] Chinese Acad Sci, Beijing Engn Res Ctr Sea Deep Drilling & Explorat, Inst Acoust, Beijing 100190, Peoples R China
基金
中国国家自然科学基金;
关键词
porous media acoustics; time-splitting staggered-grid finite-difference; plan wave analysis; propagation characteristics; ELASTIC-WAVES; ACOUSTIC PROPAGATION; ATTENUATION; MODEL;
D O I
10.7498/aps.71.20212012
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Aiming at the propagation characteristics of acoustic waves in a porous medium containing a solid in pores,the equations of motion and constitutive relation are deducted in the case of two-solid porous media. Thefrequency dispersion and attenuation characteristics of wave modes are analyzed by a plane wave analysis. Inaddition, based on the first-order velocity-stress equations, the time-splitting high-order staggered-grid finite-difference algorithm is proposed and constructed for understanding wave propagation mechanisms in such amedium, where the time-splitting method is used to solve the stiffness problem in the first-order velocity-stressequations. The generation mechanisms and energy distributions of different kinds of waves are investigated indetail. In particular, the influences of the friction coefficient between solid grains and pore solid as well asfrequency on wave propagation are analyzed. It can be known from the results of plane wave analysis that thereare two compression waves (P1 and P2) and two shear waves (S1 and S2) in a porous medium containing asolid in pores. The attenuations of P2 wave and S2 wave are much larger than those of P1 wave and S1 wave.This is due to the friction between the solid grains and the pore solid. The results show that our proposednumerical simulation algorithm can effectively solve the problem of stiffness in the velocity-stress equations,with high accuracy. The excitation mechanisms of the four wave modes are clearly revealed by the simulationresults. The P1 wave and S1 wave propagate primarily in the solid grain frame, while P2 wave and S2 wave areconcentrated mainly in the pore solid, which are caused by the relative motion between the solid grains and thepore solid. Besides, it should be pointed out that the wave diffusions of the P2 wave and S2 wave are influencedby the friction coefficient between solid grains and pore solid. The existence of friction coefficient between twosolids makes P2 wave and S2 wave attenuate to a certain extent at high frequency, but the attenuation is muchsmaller than that at low frequency. This is the reason why it is difficult to observe the slow waves in practice.However, because the slow waves also carry some energy, it may not be ignored in the studying of the energyattenuation of acoustic waves in porous media
引用
收藏
页数:13
相关论文
共 35 条
[1]   A mixed displacement-pressure formulation for poroelastic materials [J].
Atalla, N ;
Panneton, R ;
Debergue, P .
JOURNAL OF THE ACOUSTICAL SOCIETY OF AMERICA, 1998, 104 (03) :1444-1452
[2]   Biot-Rayleigh theory of wave propagation in double-porosity media [J].
Ba, J. ;
Carcione, J. M. ;
Nie, J. X. .
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH, 2011, 116
[3]   Rock anelasticity due to patchy saturation and fabric heterogeneity: A double double-porosity model of wave propagation [J].
Ba, Jing ;
Xu, Wenhao ;
Fu, Li-Yun ;
Carcione, Jose M. ;
Zhang, Lin .
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH, 2017, 122 (03) :1949-1976
[4]   Seismic attenuation due to heterogeneities of rock fabric and fluid distribution [J].
Ba, Jing ;
Carcione, Jose M. ;
Sun, Weitao .
GEOPHYSICAL JOURNAL INTERNATIONAL, 2015, 202 (03) :1843-1847
[5]   Elastic wave propagation and attenuation in a double-porosity dual-permeability medium [J].
Berryman, JG ;
Wang, HF .
INTERNATIONAL JOURNAL OF ROCK MECHANICS AND MINING SCIENCES, 2000, 37 (1-2) :63-78
[6]  
Biot M A, 1956, J ACOUST SOC AM, V28, P179
[7]  
Biot M A., 1956, J ACOUST SOC AM, V28, P168, DOI [10.1121/1.1908239, DOI 10.1121/1.1908239]
[9]   MECHANICS OF DEFORMATION AND ACOUSTIC PROPAGATION IN POROUS MEDIA [J].
BIOT, MA .
JOURNAL OF APPLIED PHYSICS, 1962, 33 (04) :1482-+
[10]  
Carcione J.M., 2001, WAVE FIELDS REAL MED