next up previous print clean
Next: Diffracted multiples Up: Kinematics of Multiples in Previous: Kinematics of Multiples in

Water-bottom multiples

Consider a model with a dipping water-bottom in 2D. The raypath of the primary reflection can be easily computed using the concept of the image source as illustrated in Figure [*].

 
rayprim
Figure 1
Construction of the primary reflection from a dipping interface.
rayprim
view burn build edit restore

The moveout of the primary reflection in the CMP domain is given by:  
 \begin{displaymath}
t_p=\sqrt{\left(\frac{2Z_D}{V}\right)^2+\left(\frac{2h_D}{V_{NMO}}\right)^2}=\sqrt{t_0^2+\left(\frac{2h_D}{V_{NMO}}\right)^2}\end{displaymath} (1)
where tp is the time of the primary, $\varphi$ is the dip angle of the reflector, ZD is the perpendicular distance between the surface and the reflector at the CMP location, hD is half the source-receiver offset, V is the propagation velocity above the dipping reflector, $V_{NMO}=V/\cos\varphi$ is the normal moveout velocity and t0 is the traveltime of the zero-offset reflection. This is obviously the equation of a hyperbola, as illustrated in Figure [*].

The raypath of the multiple reflection can be considered as a cascaded of two primary reflections as SRME methods do (Figure [*]), but the traveltime of the multiple, tm, can be computed more easily as the traveltime of an equivalent primary from a reflector dipping at twice the dip angle of the actual reflector as illustrated in Figure [*]. That is,  
 \begin{displaymath}
t_m=\sqrt{\left(\frac{2\hat{Z}_D}{V}\right)^2+\left(\frac{2h_D}{\hat{V}_{NMO}}\right)^2}\end{displaymath} (2)
where $\hat{Z}_D$ is the perpendicular distance between the surface and the equivalent reflector with twice the dip at the CMP location and $\hat{V}_{NMO}$ is now $V/\cos(2\varphi)$. Figure [*] corresponds to a CMP showing the primary and the multiple reflection. Obviously, they are both hyperbolas since the multiple has the same kinematics as a primary from a reflector dipping at twice the dip as indicated above.

 
raymul1
Figure 2
Decomposition of the water-bottom multiple as a cascaded of two primary reflections.
raymul1
view burn build edit restore

 
raymul2
Figure 3
Multiple reflection as a primary from an equivalent reflector with twice the dip angle.
raymul2
view burn build edit restore

 
moveouts1
Figure 4
Moveout curves of primary and water-bottom multiple from a dipping interface on a CMP gather.
moveouts1
view burn build edit restore


next up previous print clean
Next: Diffracted multiples Up: Kinematics of Multiples in Previous: Kinematics of Multiples in
Stanford Exploration Project
5/3/2005