Title: 3-D Modeling of Rupture Sequences of Shallow Subduction Earthquakes
1 3-D Modeling of Rupture Sequences of Shallow
Subduction Earthquakes
- Yajing Liu1, James R. Rice1,2
- 1 Department of Earth and Planetary Sciences,
Harvard University - 2 Division of Engineering and Applied Sciences,
Harvard University - AGU Fall 2003, T42C-07
2We look at
- Complexities of modeled large shallow subduction
earthquake populations - Detailed slip behaviors during modeled great
earthquakes - Aseismic transients observed from simulations.
3Geometry and modeling setup
4Rate- and state-dependent friction law(including
a single state variable, Dieterich, 1978, 1981
Ruina, 1983)
Dieterich-Ruina friction (slowness law)
- Stability determining parameters
- velocity dependence of steady state friction
- nucleation size
-
(actual size 3 4 h)
5Depth distribution of friction parameters a and
(a ? b)
Introduce along-strike non-uniformities
6Overburden total normal stress and pore pressure
- Total normal stress
- Pore pressure
- Effective normal stress(at greater
depth)
7Depth-averaged (over seismogenic zone) slip
versus x (along strike)
Lines plotted every 5 years
Event A
Starting time to compare results with two grid
resolutions
8Comparison of results from two grid resolutions
9Slip and slip velocity evolution of Event A
10Aseismic transients
11Another example
- Slip rate 10103 Vpl
- Initiate from the gap zones
- Migrate along strike near the downdip end of the
seismogenic zone at an average speed 10-5 to
10-6 of the rupture propagation speed during
great events - Not always rupture to the surface.
12Conclusions
- Small along-strike variations in material
frictional properties (or initial conditions)
could perturb the system into a non-uniform slip
mode, with large events occurring at various
locations, different recurrence intervals, and
multiple magnitudes. - With current h, and grid resolution, we observe
events with aseismic slip rates (10103 Vpl),
migrating along strike near the downdip end of
the seismogenic zone.