The velocity models are depicted in the same color scale in the upper
panels of Figures (``WEMVA works'') and
(``WEMVA breaks''). The
background velocity is 2000 m/s for both. The peak anomalies,
from left to right, as departures from the background, are (in m/s):
-153, -188, +231 for the ``WEMVA works'' velocity model and -586,
-766, +519 for the ``WEMVA breaks'' velocity model.
The ``WEMVA works'' velocity anomalies cause visible amplitude
focusing, but minimal traveltime anomalies (middle panel in Figure
). The intense ``WEMVA
breaks'' velocity lenses, on the other hand, cause visible
triplications and departures from hyperbolicity (middle panel in Figure
). The specific signature of FEAVO before migration can
be examined in both cases by squaring each of the values in the data
cube, then summing along the time axis. The results of this operation
is shown in the lower panels of Figures
and
respectively. The axes of the image are midpoint and offset, and
specific ``V'' shapes are visible for each of the three velocity
anomalies.
It is interesting to compare these FEAVO effects with those present in
the only field dataset currently available to us that exhibits FEAVO
anomalies. The dataset in question is the Grand Isle dataset analyzed
by Kjartansson (1979) - the original dataset on which FEAVO was
defined. The FEAVO effects in it are comparable with those in the
lower panels of Figures and
because the
background velocities are approximately similar. Given that the
intensity of the effects is linked to the magnitude of the velocity
anomalies, we can empirically estimate that the deviation of the Grand
Isle velocity anomalies from the background is around 200-300
m/s. Since the ``thickness'' of the V's is linked to the
dimensions of the velocity lenses, we can also infer that they are
approximately 20-30m in diameter.
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