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The RMO functions derived above can be directly used in a
layered-based vertical updating of the velocity function
after migration.
However, in complex media it is often desirable to invert the depth errors
measured from ADCIGs into velocity-parameters perturbations
through a tomographic procedure.
To be able to apply a tomographic method,
we must perform an additional step to convert
the depth errors measured from ADCIGs into
traveltime errors.
This depth-to-time conversion can be easily
accomplished by slightly rewriting the chain of
partial derivatives in equation 35,
and obtain the following relationship:
| ![\begin{displaymath}
\frac{\partial z_\gamma}{\partial t}
=
\frac{\partial z_\gam...
...mma+ \sin \gamma\tan \widetilde{\gamma}}{S\left(\gamma\right)},\end{displaymath}](img82.gif) |
(46) |
which can be directly applied to
convert depth errors into traveltime perturbations
to be used in tomography.
Next: Conclusions
Up: Anisotropic residual moveout for
Previous: Arbitrary scaling of velocity
Stanford Exploration Project
5/3/2005