We computed three FDPs for three different 3D Santa Clara Valley
velocity models. The first model is the San Francisco Bay Area model
from USGS (USGS Bay Area Velocity Model 05.1.0). The second model is
the UC Berkeley (UCB) 3D model (Stidham et al., 1999). The
third model is a modified USGS model. In this modified velocity
model, in order to enhance the effect due to the basin structure, we
kept the velocity structure inside the basin, but assumed only 1D
reference velocity structure for the regions outside of the basin.
The comparison between synthetic and observed FDPs shows that FDPs
for USGS and modified USGS models follow a similar depth dependent
trend as observed FDPs, and their absolute values are in agreement
as well (Figure 2.17). The synthetic FDPs for the UCB model show that FDP
correlates with basin depth up to 2 km, but the correlation
coefficient is not high and individual values are more scattered
than in the case of the other models, especially for shallow depths. We also cannot match the observed shift of the trend in
the observed FDP curve at around 2 to 3 km depth because the maximum
thickness of the basin obtained in the UCB model is only 2 km.
The observation and synthetic results show that the variations in
FDP are sensitive to the thickness of the basin up to a certain
depth and then becomes stable. The simulation of the P-wave time
delays from teleseismic events for the USGS 3D velocity model at
SCVSE stations shows a similar saturating trend as the FDPs for the
USGS model (Dolenc et al., 2005). Synthetic time delay increases
with increasing basin thickness up to a certain depth and then
stabilizes. Since the P-wave time delay depends entirely on the
mean velocity and thickness of the basin, this indicates that
velocity contrast between the basin and the background medium is
negligible at deeper depth, which is true for USGS 3D velocity
model. In the case of the Santa Clara Valley model, FDP is only
sensitive to the shallow structure, and the apparent thickness of the
deeper part of the basin is much shallower than the model. It is
likely due to the negligible velocity contrast in Santa Clara Valley
model. But we still need more experiments to confirm which factor
really controls the depth of the change in the depth-dependent trend
of the FDP.
Figure 2.17:
A comparison among
observed (open circles)) and three synthetic FDPs for USGS (Open
squares), modified USGS (Solid circles) and UCB (Gray triangles), as a function of depth.