Page 310 - Acquisition and Processing of Marine Seismic Data
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5.9 f-k DIP FILTERS                           301

              As explained in Section 4.6, the f-k spectrum  spectrum. Essentially, the f-k filter is one of the
           consists of two panels: one is negative and other  most efficient and commonly used methods in
           is a positive panel, represented by negative and  removing the ground-roll noise from land shot
           positive wavenumbers against the frequency,  gathers.
           respectively (Fig. 5.65). In marine shot gathers,  The 2D Fourier transform enables us to filter
           the positive panel involves the amplitudes of  the seismic data in 2D and to suppress some spe-
           primary and multiple reflections, direct wave  cific correlated noise types. Basically, the pro-
           and refractions, while the negative panel com-  cess is as follows (Fig. 5.66): the f-k spectrum is
           prises spatially aliased signals, back-scattered  calculated by computing the 2D Fourier trans-
           amplitudes and the events with negative dip,  form of the input seismic data. Amplitudes of
           such as tail buoy noise. Bird noise and mechan-  the events with different dips (or different prop-
           ical cable noise amplitudes are located in both  agation velocities) accumulate in different areas
           panels. In general, it is not possible to recognize  on the f-k panel according to their wavenumbers
           the amplitudes of multiple reflections as an iso-  and frequencies. In order to remove a particular
           lated amplitude package in the f-k spectra. In  event in the time domain data, for instance the
           land seismic shot gathers, however, direct and  ground-roll in land seismic data, the area in
           refracted wave amplitudes, as well as air waves,  the f-k domain that contains the amplitudes of
           appear in both panels of the f-k spectrum. In  that particular event is multiplied by a small
           addition, surface waves, known as ground-roll,  coefficient close to zero. The reason that the
           are quite dominant on the f-k spectra, and their  amplitudes are not multiplied by zero is based
           respective amplitudes are prominent packages  on the Fourier theory: If we multiply the ampli-
           isolated from the primary reflections close to  tude spectrum by a constant in the frequency
           the wavenumber axis of both panels in the f-k  domain, this means that the function is scaled






























           FIG. 5.65  Negative and positive panels of an f-k spectrum and f-k domain appearance of common events encountered in
           marine shot gathers.
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