Finite element modelling of frictional instability between deformable rocks
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[1] B. Shibazaki,et al. Slip-dependent friction law and nucleation processes in earthquake rupture , 1992 .
[2] W. Brace,et al. Stick-Slip as a Mechanism for Earthquakes , 1966, Science.
[3] P. Bird,et al. Thin‐shell modeling of neotectonics in the Azores‐Gibraltar Region , 2001 .
[4] Huilin Xing,et al. FE modeling of thermo‐elasto‐plastic finite deformation and its application in sheet warm forming , 2002 .
[5] Tao He,et al. Numerical Simulation of Dynamic Process of the Tangshan Earthquake by a New Method—LDDA , 2000 .
[6] J. A. Snoke,et al. Topographic and seismic effects of long-term coupling between the subducting and overriding plates beneath Northeast Japan , 1997 .
[7] G. P. Nikishkov,et al. Static-explicit FE modeling of 3-d large deformation multibody contact problems on parallel computer , 1998 .
[8] Huilin Xing,et al. Numerical analysis and design for tubular hydroforming , 2001 .
[9] Tomowo Hirasawa,et al. A numerical study on seismic coupling along subduction zones using a laboratory-derived friction law , 1997 .
[10] C. Scholz. Earthquakes and friction laws , 1998, Nature.
[11] J. Dieterich. Modeling of rock friction: 1. Experimental results and constitutive equations , 1979 .
[12] A. Curnier,et al. A finite element method for a class of contact-impact problems , 1976 .
[13] Effect of fault bend on the rupture propagation process of stick-slip , 1999 .
[14] David R. O'Hallaron,et al. Large-scale simulation of elastic wave propagation in heterogeneous media on parallel computers , 1998 .
[15] Richard E. Goodman,et al. Two dimensional discontinuous deformation analysis , 1985 .
[16] C. Marone. LABORATORY-DERIVED FRICTION LAWS AND THEIR APPLICATION TO SEISMIC FAULTING , 1998 .
[17] GEOFFREY KING,et al. Role of Fault Bends in the Initiation and Termination of Earthquake Rupture , 1985, Science.
[18] S. Cloetingh,et al. Finite-element modelling of stress patterns along the Mid-Norwegian continental margin, 62° to 68°N , 1996 .
[19] D. J. Andrews,et al. Rupture propagation with finite stress in antiplane strain , 1976 .
[20] M. Ohnaka,et al. Scaling of the shear rupture process from nucleation to dynamic propagation: Implications of geometric irregularity of the rupturing surfaces , 1999 .
[21] William D. Stuart,et al. Forecast model for great earthquakes at the Nankai Trough subduction zone , 1988 .
[22] J. C. Simo,et al. An augmented lagrangian treatment of contact problems involving friction , 1992 .
[23] P. Bird. Finite element modeling of lithosphere deformation: The Zagros collision orogeny , 1978 .
[24] A. Ruina. Slip instability and state variable friction laws , 1983 .
[25] John R. Rice,et al. Dynamic motion of a single degree of freedom system following a rate and state dependent friction law , 1986 .
[26] R. Koeller,et al. A non-equilibrium thermodynamic theory of flow through deformable porous media , 1978 .
[27] C. Scholz. The Mechanics of Earthquakes and Faulting , 1990 .
[28] J. Dieterich. Time-dependent friction and the mechanics of stick-slip , 1978 .
[29] Mitiyasu Ohnaka,et al. Constitutive relations between dynamic physical parameters near a tip of the propagating slip zone during stick-slip shear failure , 1987 .
[30] H. Xing,et al. Three dimensional finite element modeling of thermomechanical frictional contact between finite deformation bodies using R-minimum strategy , 2002 .
[31] H. Melosh,et al. Mechanics of graben formation in crustal rocks - A finite element analysis , 1989 .
[32] Genki Yagawa,et al. Nonlinear Structural Subsystem of GeoFEM for Fault Zone Analysis , 2000 .