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NMO

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 $F_W M_{\mbox{\rm\scriptsize NMO}}$,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} (25)

The anellipticity parameter FW controls the deviation from normal moveout; if $F_W \equiv 1$ the moveout is exactly hyperbolic. Note that one should not try to define $F_W = M_x / M_{{\mbox{\rm\scriptsize NMO}}}$using a measured value for Mx. FW and $M_{{\mbox{\rm\scriptsize NMO}}}$are both vertical paraxial measurements; there is no reason to suppose they should be strictly related to Mx, a horizontal measurement.



 
previous up next print clean
Next: Dix's equation Up: Dellinger, Muir, & Karrenbach: Previous: Approximating TI dispersion relations
Stanford Exploration Project
11/17/1997