Next: Dix's equation
Up: Dellinger, Muir, & Karrenbach:
Previous: Approximating TI dispersion relations
The first-anelliptic example in Figure
would have been more realistic if we had simply omitted
the depth scale entirely.
Mathematically this means rewriting
equation (
) explicitly in terms of vertical traveltime,
finding the first-anelliptic equivalent of equation (
).
To do this,
replace Mz C by T(0)2,
S by x2,
and
Mx by
,obtaining the first-anelliptic processing-NMO equation:
| ![\begin{displaymath}
T(x)^2 =
{{
T(0)^4
+
( F_W + 1 )
T(0)^2 M_{\mbox{\rm\scripts...
...2 x^4
\over
T(0)^2 + F_W M_{\mbox{\rm\scriptsize NMO}} x^2
}}
.\end{displaymath}](img63.gif) |
(25) |
The anellipticity parameter FW controls the deviation from
normal moveout; if
the moveout is exactly hyperbolic.
Note that one should not try to define
using a measured value for Mx.
FW and
are both vertical paraxial measurements;
there is no reason to suppose
they should be strictly related to Mx, a horizontal measurement.
Next: Dix's equation
Up: Dellinger, Muir, & Karrenbach:
Previous: Approximating TI dispersion relations
Stanford Exploration Project
11/17/1997