Page 399 - Acquisition and Processing of Marine Seismic Data
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390                          7. SUPPRESSION OF MULTIPLE REFLECTIONS
































           FIG. 7.24  A brute stack section (A) before and (B) after Radon velocity filter. Amplitudes below the acoustic basement in
           (A) represent interbed multiples.


           manner. According to this signal propagation  assumed that the seafloor is horizontal for each
           geometry, the signal recorded at receiver R 3  individual shot. Seabed reflection is picked from
           can be used to estimate the record at R 6 , and sim-  brute stack sections and the arrival time of this
           ilarly, the record at receiver R 6 can be used to  reflection is converted into depth using average
           estimate the record at R 8 , and so on. The follow-  wave velocity in the water. If the seabed is
           ing information can then be deduced from this  inclined, the data can be migrated using a fast
           signal propagation geometry (Wiggins, 1988):  migration algorithm, such as the Stolt f-k migra-
                                                        tion using a constant velocity. In addition, since
             i. Reflection  from  sea  surface:  used  to
                                                        the reflection coefficient of the seabed cannot be
               determine surface reflection coefficient.
                                                        obtained from the seismic data, it is calculated in
            ii. Propagation to the seabed: used to obtain
                                                        a statistical fashion.
               travel time to the seafloor, and amplitude
                                                           Fig. 7.26A shows a stack section from a shal-
               loss due to the spherical divergence.
                                                        low continental shelf with a horizontal seafloor
           iii. Reflection from seabed: used to calculate
                                                        consisting of a nice stratigraphy over a regional
               seabed reflection coefficient statistically.
                                                        basement high. The section also includes both
            iv. Propagation to the receiver: used to obtain
                                                        long period and peg-leg multiples indicated by
               travel time to the receiver, and amplitude
                                                        M, which are especially distinct below the base-
               loss due to the spherical divergence.
                                                        ment high at the lefthand side where there are no
              Reflection from the seabed and propagation  primary reflections. Fig. 7.26B shows the multi-
           to a receiver require that the seabed already be  ple energy modeled by WEMR, which is then
           defined in time and distance dimensions along  subtracted from the input data to obtain the out-
           the line. For simplicity in computations, it is  put section in Fig. 7.26C. The output stack
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