Page 308 - Acquisition and Processing of Marine Seismic Data
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5.9 f-k DIP FILTERS                           299




























           FIG. 5.63  Effect of top mute ramp on the seabed reflection. (A) Example stack section with no top mute. Same section after
           top muting with ramp values of (B) 0 ms, (C) 5 ms, (D) 10 ms, (E) 20 ms, and (F) 30 ms. The ramped unit step functions mul-
           tiplied by the seismic data are indicated by heavy red lines. The longer the mute ramp length, the higher the suppression of the
           seabed reflection amplitudes.



           of the ramp length on the seabed reflection ampli-  Dip filtering uses a 2D Fourier transform to
           tudes. As the ramp value increases, the ampli-  remove certain types of correlated noise propa-
           tudes of the seabed reflections are increasingly  gating with different velocities, which appear as
           suppressed after muting, which can result in  events with different dips on the seismic data.
           issues in autopicking during the interpretation  As explained in Section 4.6, a 2D forward
           stage. As a rule of thumb, the ramp value should  Fourier transform converts the seismic data
           not exceed one-third of the dominant period of  from the time-distance (t-x) domain into the
           the seismic wavelet, to avoid excessive amplitude  frequency-wavenumber (f-k) domain, and thus
           reduction along the seafloor reflection.     the result of a 2D Fourier transform of the seis-
                                                        mic data is known as the f-k spectrum. The
                                                        amplitudes of certain correlated events in the
                     5.9 f-k DIP FILTERS                time domain appear at specific points on the cor-
                                                        responding f-k spectrum. This may allow us to
              Shot gathers and stack sections have corre-  discriminate the noise and signal amplitudes
           lated events of different dips consisting of coher-  in the f-k domain. Fig. 5.64 shows the schematic
           ent noise and primary reflections. For instance,  illustration of the common events that can be
           direct waves and refractions appear as linear  observed on a marine shot gather and their fre-
           correlated events extending from near to far  quency domain appearance after a 2D Fourier
           offsets on the shot records, whereas primary  transform.
           reflections and their multiples are in the form  The f-k spectrum is a powerful tool to dis-
           of hyperbolic events of relatively lower dip.  criminate the correlated events with different
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