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Representation of a velocity analysis panel

The CMP gather G can be viewed as a sum of gathers Gtx, each containing only one non-zero amplitude:
\begin{displaymath}
G = \sum_{t,x} A(t,x) G_{tx},\end{displaymath} (4)
where Gtx is a gather containing a spike at (t,x) and A(t,x) is the amplitude of a trace with offset x at time t.

Because the image of Gtx is a $(\tau,m)$-space containing a parabola, we can write
\begin{displaymath}
V = \sum_{t,x} A(t,x) V_{tx},\end{displaymath} (5)
i.e., the $(\tau,m)$-space can be viewed as a sum of panels, each containing one parabola. For a constant offset x, the resulting sets of parabolas are shown in Figure [*].

Let us denote as Vx the panel that we get for one offset x:
\begin{displaymath}
V_x = \sum_t A(t,x) V_{tx}.\end{displaymath} (6)
Vx is an image of a trace with offset x. Finally we have
\begin{displaymath}
V=\sum_x V_x.\end{displaymath} (7)
Vx consists of horizontal lines for x=0. For increasing offset Vx consists of parabolas with increasing slopes (Figure [*]).


next up previous print clean
Next: The slopes of the Up: STRUCTURE OF A VELOCITY Previous: Image of a point
Stanford Exploration Project
1/13/1998