Wave propagation in thermo-poroelasticity: A finite-element approach

被引:0
作者
Santos, Juan Enrique [1 ,2 ,3 ]
Carcion, Jose Mario [1 ,4 ]
Savioli, Gabriela Beatriz [2 ]
Ba, Jing [1 ]
机构
[1] Hohai Univ, Sch Earth Sci & Engn, Nanjing, Peoples R China
[2] Univ Buenos Aires, Fac Ingn, Inst Gas & Petr, Buenos Aires, Argentina
[3] Purdue Univ, Dept Math, W Lafayette, IN USA
[4] Natl Inst Oceanog & Appl Geophys, OGS, Sgon, TS, Italy
关键词
THERMOELASTIC ATTENUATION;
D O I
10.1190/GEO2022-0271.1
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
We have developed continuous and discrete-time finite-element (FE) methods to solve an initial boundary-value problem for the thermo-poroelasticity wave equation based on the combined Biot/Lord-Shulman (LS) theories to describe the porous and thermal effects, respectively. In particular, the LS model, which includes a Maxwell-Vernotte-Cattaneo relaxation term, leads to a hyperbolic heat equation, thus avoiding infinite signal velocities. The FE methods are formulated on a bounded domain with absorbing boundary conditions at the artificial boundaries. The dynamical equations predict four propagation modes, a fast P (P1) wave, a Biot slow (P2) wave, a thermal (T) wave, and a shear (S) wave. The spatial discretization uses globally continuous bilinear polynomials to represent solid displacements and temperature, whereas the vector part of the Raviart-Thomas-Nedelec of zero order is used to represent fluid displacements. First, a priori optimal error estimates are derived for the continuous-time FE method, and then an explicit conditionally stable discrete-time FE method is defined and analyzed. The explicit FE algorithm is implemented in one dimension to analyze the behavior of the P1, P2, and T waves. The algorithms can be useful for a better understanding of seismic waves in hydrocarbon reservoirs and crustal rocks, whose description is mainly based on the assumption of isothermal wave propagation.
引用
收藏
页码:WA161 / WA175
页数:15
相关论文
共 25 条
[1]  
Adams R.A., 2003, Sobolev Spaces, Vsecond
[2]   MODELS FOR THERMOELASTIC ATTENUATION OF WAVES IN HETEROGENEOUS SOLIDS [J].
ARMSTRONG, BH .
GEOPHYSICS, 1984, 49 (07) :1032-1040
[3]   THERMOELASTICITY AND IRREVERSIBLE THERMODYNAMICS [J].
BIOT, MA .
JOURNAL OF APPLIED PHYSICS, 1956, 27 (03) :240-253
[4]  
Carcione J. M., 2022, Wave fields in real media: Wave propagation in anisotropic, anelastic, porous and electromagnetic media, V4th
[5]   Canonical analytical solutions of wave-induced thermoelastic attenuation [J].
Carcione, Jose M. ;
Gei, Davide ;
Santos, Juan E. ;
Fu, Li-Yun ;
Ba, Jing .
GEOPHYSICAL JOURNAL INTERNATIONAL, 2020, 221 (02) :835-842
[6]   Physics and Simulation of Wave Propagation in Linear Thermoporoelastic Media [J].
Carcione, Jose M. ;
Cavallini, Fabio ;
Wang, Enjiang ;
Ba, Jing ;
Fu, Li-Yun .
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH, 2019, 124 (08) :8147-8166
[7]   Simulation of wave propagation in linear thermoelastic media [J].
Carcione, Jose M. ;
Wang, Zhi-Wei ;
Ling, Wenchang ;
Salusti, Ettore ;
Ba, Jing ;
Fu, Li-Yun .
GEOPHYSICS, 2019, 84 (01) :T1-T11
[8]  
Duvaut G., 1976, Inequalities in Mechanics and Physics
[9]  
Girault V., 1981, Finite Element Approximation of the Navier-Stokes Equations, Lectures Notes in Mathematics 749
[10]   Thermoelastic damping in micro- and nanomechanical systems [J].
Lifshitz, R ;
Roukes, ML .
PHYSICAL REVIEW B, 2000, 61 (08) :5600-5609