Seismoelectric numerical simulation in 2D vertical transverse isotropic poroelastic medium

Journal Article (2020)
Author(s)

Munirdin Tohti (Chinese Academy of Sciences)

Yibo Wang (Chinese Academy of Sciences)

E.C. Slob (TU Delft - Applied Geophysics and Petrophysics)

Yikang Zheng (Chinese Academy of Sciences)

Xu Chang (Chinese Academy of Sciences)

Yi Yao (Chinese Academy of Sciences)

Research Group
Applied Geophysics and Petrophysics
Copyright
© 2020 Munirdin Tohti, Yibo Wang, E.C. Slob, Yikang Zheng, Xu Chang, Yi Yao
DOI related publication
https://doi.org/10.1111/1365-2478.12958
More Info
expand_more
Publication Year
2020
Language
English
Copyright
© 2020 Munirdin Tohti, Yibo Wang, E.C. Slob, Yikang Zheng, Xu Chang, Yi Yao
Research Group
Applied Geophysics and Petrophysics
Issue number
6
Volume number
68
Pages (from-to)
1927-1943
Reuse Rights

Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons.

Abstract

Seismoelectric coupling in an electric isotropic and elastic anisotropic medium is developed using a primary–secondary formulation. The anisotropy is of vertical transverse isotropic type and concerns only the poroelastic parameters. Based on our finite difference time domain algorithm, we solve the seismoelectric response to an explosive source. The seismic wavefields are computed as the primary field. The electric field is then obtained as a secondary field by solving the Poisson equation for the electric potential. To test our numerical algorithm, we compared our seismoelectric numerical results with analytical results obtained from Pride's equation. The comparison shows that the numerical solution gives a good approximation to the analytical solution. We then simulate the seismoelectric wavefields in different models. Simulated results show that four types of seismic waves are generated in anisotropic poroelastic medium. These are the fast and slow longitudinal waves and two separable transverse waves. All of these seismic waves generate coseismic electric fields in a homogenous anisotropic poroelastic medium. The tortuosity has an effect on the propagation of the slow longitudinal wave. The snapshot of the slow longitudinal wave has an oval shape when the tortuosity is anisotropic, whereas it has a circular shape when the tortuosity is isotropic. In terms of the Thomsen parameters, the radiation anisotropy of the fast longitudinal wave is more sensitive to the value of ε, while the radiation anisotropy of the transverse wave is more sensitive to the value of δ.

Files

1365_2478.12958.pdf
(pdf | 9.6 Mb)
- Embargo expired in 13-10-2020
License info not available