Page 237 - Acquisition and Processing of Marine Seismic Data
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228                          4. FUNDAMENTALS OF DATA PROCESSING


























           FIG. 4.15  (A) A synthetic zero offset section with four dipping events indicated by A, B, C, and D, and its f-k spectra for
           (B) 2 m, (C) 5 m, and (D) 10 m trace interval. Spatially aliased event amplitudes are indicated in red on the f-k spectra.

           wavelet. In the f-k panel for the section of the 2-m  since it represents incorrect dips in the time
           trace interval in Fig. 4.15B, amplitudes of all dip-  domain. The maximum unaliased frequency
           ping events appear as straight lines passing  on an f-k spectrum F u can be calculated by
           through the origin and there is no spatial alias-                   V
           ing in the f-k spectrum. If we recompute the time            F u ¼ 2Δxsinθ         (4.19)
           section with a 5-m trace interval, inclinations of
           all straight lines increase and the amplitudes of  where Δx is the trace interval, V is the velocity of
           the events A and D with extreme dip are spa-  the medium,andθ is theinclination of theeventin
           tially aliased in the f-k spectrum (Fig. 4.15C).  the time domain. Eq. (4.19) suggests that the
           For a 10-m trace interval, only the amplitudes  higherthedipontimesections,thelowerthealias-
           of event B with the smoothest dip are not aliased  ing frequency in the f-k domain. Similarly, the
           in the f-k spectrum, while the amplitudes of  higher the trace interval in the time domain, the
           event D are aliased twice (Fig. 4.15D).      lower the aliasing frequency in the f-k domain.
              In the 2D Fourier spectrum of the seismic    Fig. 4.16A shows a real shot gather with its f-k
           data, spatial aliasing is often pronounced,  spectrum. The data has 96 traces with 6.25 m
           depending on the trace interval of the input  trace interval. The f-k spectrum of the shot indi-
           data. The Nyquist wavenumber, k N , determines  cates that the components higher than approxi-
           the aliasing wavenumber, which is            mately 120 Hz are spatially aliased. Fig. 4.16B
                                                        and C show the same shot but decimated to
                                  1
                             k N ¼               (4.18)  obtain shot records with 48 (12.5 m group inter-
                                 2Δx
                                                        val) and 32 (18.75 m group interval) traces,
           where Δx is the spatial sampling interval (or  respectively. The aliasing frequency of the f-k
           trace interval of the input). Wavenumbers larger  spectra decreases to 60 Hz for the shot with
           than the Nyquist wavenumber will simply alias  12.5 m and 40 Hz for the shot with 18.75 m group
           in the f-k domain. An aliased signal is undesired  interval. Furthermore, the amplitudes of the
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