Earthquake cycle simulations with rate-and-state friction and power-law viscoelasticity

被引:67
作者
Allison, Kali L. [1 ]
Dunham, Eric M. [1 ,2 ]
机构
[1] Stanford Univ, Dept Geophys, Stanford, CA 94305 USA
[2] Stanford Univ, Inst Computat & Math Engn, Stanford, CA 94305 USA
基金
美国国家科学基金会;
关键词
Earthquake cycle; Viscoelastic flow; Power-law rheology; Strike-slip; Brittle-ductile transition; Rate-and-state friction; Summation-by-parts operators; STRIKE-SLIP-FAULT; SAN-ANDREAS FAULT; FINITE-DIFFERENCE APPROXIMATIONS; EFFECTIVE ELASTIC THICKNESS; UPPER-MANTLE; FLOW LAWS; CRUSTAL STRUCTURE; HEAT-FLOW; CONTINENTAL LITHOSPHERE; GEODETIC OBSERVATIONS;
D O I
10.1016/j.tecto.2017.10.021
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 simulate earthquake cycles with rate-and-state fault friction and off-fault power-law viscoelasticity for the classic 2D antiplane shear problem of a vertical, strike-slip plate boundary fault. We investigate the interaction between fault slip and bulk viscous flow with experimentally-based flow laws for quartz-diorite and olivine for the crust and mantle, respectively. Simulations using three linear geotherms (dT/dz = 20, 25, and 30 K/km) produce different deformation styles at depth, ranging from significant interseismic fault creep to purely bulk viscous flow. However, they have almost identical earthquake recurrence interval, nucleation depth, and down-dip coseismic slip limit. Despite these similarities, variations in the predicted surface deformation might permit discrimination of the deformation mechanism using geodetic observations. Additionally, in the 25 and 30 K/km simulations, the crust drags the mantle; the 20 K/km simulation also predicts this, except within 10 km of the fault where the reverse occurs. However, basal tractions play a minor role in the overall force balance of the lithosphere, at least for the flow laws used in our study. Therefore, the depth-integrated stress on the fault is balanced primarily by shear stress on vertical, fault-parallel planes. Because strain rates are higher directly below the fault than far from it, stresses are also higher. Thus, the upper crust far from the fault bears a substantial part of the tectonic load, resulting in unrealistically high stresses. In the real Earth, this might lead to distributed plastic deformation or formation of subparallel faults. Alternatively, fault pore pressures in excess of hydrostatic and/or weakening mechanisms such as grain size reduction and thermo-mechanical coupling could lower the strength of the ductile fault root in the lower crust and, concomitantly, off-fault upper crustal stresses.
引用
收藏
页码:232 / 256
页数:25
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