Model for the Bipolar Amplification Effect

Author(s):  
James P. Ashton ◽  
Stephen J. Moxim ◽  
Ashton D. Purcell ◽  
Patrick M. Lenahan ◽  
Jason T. Ryan
2021 ◽  
Vol 130 (13) ◽  
pp. 134501
Author(s):  
James P. Ashton ◽  
Stephen J. Moxim ◽  
Ashton D. Purcell ◽  
Patrick M. Lenahan ◽  
Jason T. Ryan

2015 ◽  
Vol 15 (4) ◽  
pp. 595-603 ◽  
Author(s):  
Song Ruiqiang ◽  
Chen Shuming ◽  
Du Yankang ◽  
Huang Pengcheng ◽  
Chen Jianjun ◽  
...  

2012 ◽  
Vol 21 (1) ◽  
pp. 016103 ◽  
Author(s):  
Jian-Jun Chen ◽  
Shu-Ming Chen ◽  
Bin Liang ◽  
Ke-Feng Deng

2010 ◽  
Vol 59 (1) ◽  
pp. 649
Author(s):  
Liu Zheng ◽  
Chen Shu-Ming ◽  
Liang Bin ◽  
Liu Bi-Wei ◽  
Zhao Zhen-Yu

2017 ◽  
Vol 25 (4) ◽  
pp. 662 ◽  
Author(s):  
Zuo-Jun WANG ◽  
Yi-Ru HOU ◽  
Yi KUANG ◽  
Hui-Yi TANG ◽  
Zhen-Zhen ZHAO ◽  
...  
Keyword(s):  

2015 ◽  
Vol 24 (11) ◽  
pp. 119401 ◽  
Author(s):  
Jun-Ting Yu ◽  
Shu-Ming Chen ◽  
Jian-Jun Chen ◽  
Peng-Cheng Huang

Author(s):  
Gabriel Malagon-Carvajal ◽  
Cesar Duarte ◽  
Gabriel Ordonez-Plata ◽  
C F M Almeida ◽  
Nelson Kagan
Keyword(s):  

2008 ◽  
Vol 20 (16) ◽  
pp. 1748-1753 ◽  
Author(s):  
Jenny Gun ◽  
Michael J. Schöning ◽  
Maryam H. Abouzar ◽  
Arshak Poghossian ◽  
Evgeny Katz

Author(s):  
Zhongxian Liu ◽  
Jiaqiao Liu ◽  
Sibo Meng ◽  
Xiaojian Sun

Summary An indirect boundary element method (IBEM) is developed to model the two-dimensional (2D) diffraction of seismic waves by a fluid-filled crack in a fluid-saturated poroelastic half-space, using Green's functions computed considering the distributed loads, flow, and fluid characteristics. The influence of the fluid-filled crack on the diffraction characteristics is investigated by analyzing key parameters, such as the excitation frequency, incident angle, crack width and depth, and medium porosity. The results for the fluid-filled crack model are compared to those for the fluid-free crack model under the same conditions. The numerical results demonstrate that the fluid-filled crack has a significant amplification effect on the surface displacements, and that the effect of the depth of the fluid-filled crack is more complex compared to the influence of other parameters. The resonance diffraction generates an amplification effect in the case of normally incident P waves. Furthermore, the horizontal and vertical displacement amplitudes reach 4.2 and 14.1, respectively. In the corresponding case of the fluid-free crack, the vertical displacement amplitude is only equal to 4.1, indicating the amplification effect of the fluid in the crack. Conversely, for normally incident SV waves at certain resonance frequencies, the displacement amplitudes above a fluid-filled crack may be lower than the displacement amplitudes observed in the corresponding case of a fluid-free crack.


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