M. Heimpel et P. Olson, A SEISMODYNAMICAL MODEL OF LITHOSPHERE DEFORMATION - DEVELOPMENT OF CONTINENTAL AND OCEANIC RIFT NETWORKS, J GEO R-SOL, 101(B7), 1996, pp. 16155-16176
Seismicity and lithosphere extension on the scale of a tectonic plate
are investigated in two horizontal dimensions and time using a dynamic
al model for a thin plate overlying a viscoelastic channel, The plate
consists of two layers, a brittle elastic-plastic crust that deforms a
s a result of earthquakes along faults and a strong viscoelastic layer
representing the aseismic, creeping lower lithosphere. Numerical expe
riments of lithosphere rifting are performed for one- and two-layer li
thosphere models using two different rupture criteria, In all the calc
ulations, earthquakes and faults of various sizes may form anywhere in
the numerical domain as a result of the constitutive formulation. The
differences between the one-and two-layer model results suggest a mec
hanical explanation for the difference between continental and oceanic
rifting. When the lower lithosphere is absent, a small number of faul
ts dominate the deformation, and a relatively simple, narrow rift zone
develops corresponding to oceanic rifting. When a highly viscous lowe
r Lithosphere is included a complex, distributed network of faults dev
elops, similar to continental rifting, The complexity of the fault sys
tem also depends on the yield criterion in the crystal layer. In our s
imulations, complexity is greater for a yield criterion with strong sh
ear stress dependence than for one with. mainly extensional stress dep
endence, Whether a result of lower lithosphere stretching, crustal het
erogeneity, or the yield criterion, higher complexity increases the ti
mescale for fault development, increases self-similarity in fault syst
em geometry and stress and strain time series, and results in power la
w moment-frequency earthquake size scaling.