The results presented on Figure 6.6 and in Table 6.3 can be divided into 3 categories:
In order to interpret these results, we calculate the expected
surface coseismic displacements using a dislocation model in a
uniform half-space. The model parameters are the geometry of the
rupture (length, width, dip angle), its geographic location,
its depth, and the slip distribution on the rupture plane.
The dip angle (15 degrees) and fault strike (121
) are taken
from the Harvard CMT solution.
We assume a rupture length of 25 km, a width of 11.5 km, and
a uniform slip of 50 cm, purely dip-slip.
These parameters are taken from the empirical scaling laws of
Smith and Coppersmith (1994) that we slightly adjusted to match
the observed seismic moment (4.8
10
N.M).
We then adjust the location and depth of the rupture plane
by trial-and-error in order to best match coseismic offsets
at sites REUN, HIDA, and CAMP. We find that the best fit is
obtained with the center of the top portion of the rupture
located at -70.65/19.90 at a 2 km depth (Figure 7.1).
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The model on Figure 7.1 shows a good agreement with the direction of the observed coseismic displacements at sites REUN, HIDA, CAMP, and SAGO. The agreement is fair in magnitude also, although the model tends to underestimate the oberved displacements.