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We use the ray-tracing to predict the localization of the energy
in the synthetic dataset migrated with the wrong velocity.
The ray-tracing is illustrated by Figure
.
Starting from the true position of the image point
(the diamond on the Figure), we seek the position
of the image point (stars on the figure) when an incorrect migration velocity is used.
The reflector has a fixed azimuth and dip.
We first model the events recorded at the surface at one particular
aperture and reflection azimuth.
Once the true events are known, the source and the receiver rays
are shot in a media with an incorrect velocity this time.
If the velocity is too slow, then the rays stop at two
distinct end points. Knowing the position of the end points and
the ray parameters, the position of the image point in the angle domain
for an incorrect migration velocity is determined through
a geometric construction similar to the one in
.
It is also possible to use the normal shift described in the 2-D
case since we have shown
that the 3-D problem can be recast as 2-D one.
We test this procedure on an image point on
the 60 dip reflector and whose location is (400,400,1300)
in image. We choose a source-receiver pair such as the aperture angle
is
. Again, our goal is to find where the true image point
has moved because of the use of an incorrect migration velocity.
We observe on Figure
that the coordinates
of the apparent image point in the angle domain computed by ray-tracing do match
those of the image point in the model migrated with the wrong velocity.
cube_0_I0
Figure 10 Dataset migrated with the
incorrect velocity.
Next: Conclusions
Up: Synthetic example
Previous: Behavior of the reflection
Stanford Exploration Project
10/14/2003