Page 28 - Acquisition and Processing of Marine Seismic Data
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1.2 MARINE ACOUSTIC METHODS                          19






















           FIG. 1.12  (A) A 3.5 kHz Chirp transducer array ready for an over-the-side mounting; (B) an example Chirp record. The
           penetration of Chirp data is approximately 50 m.
              Boomers generate an acoustic signal between  signal has no side lobes and does not oscillate,
           approximately 1 and 6 kHz. They have capaci-  its resolution is quite high.
           tors to store the energy until shooting, and at
           each shot point, the stored energy is discharged  1.2.4 Single Channel and Multichannel
           through a spiral coil, which flexes a copper plate  Seismics
           attached to the coil to produce a stable high-
           frequency seismic signal. Boomer sources are    Conventional single- and multichannel seis-
           mounted either on a catamaran towed behind   mic methods utilize much higher amplitude
           the vessel, or on a tow-fish.                acoustic signals at relatively lower frequency
              Normally,  large  transducer  arrays  are  bands. Therefore, they have much more penetra-
           required to produce a narrow beam in subbot-  tion depth than subbottom profilers, although
           tom profiler frequency bands of 1–10 kHz. To  their resolution is relatively lower. Today, the
           overcome this issue, nonlinear acoustic systems,  conventional seismic method is the primary tool
           termed parametric systems, are used. Paramet-  for offshore hydrocarbon exploration, mapping
           ric systems enable us to produce a narrow    of shallow and deep stratigraphy, and structural
           source signal using relatively small-size trans-  setting (Table 1.6).
           ducers. In parametric sounding, two different   If we put a receiver next to the seismic source
           high-frequency acoustic signals (f 1 and f 2 ), called  and start recording at that receiver after each
           primary frequencies, are emitted into the water  shot, we can obtain true zero-offset seismic data
           column simultaneously. Nonlinear interference  when we move this system along a straight sur-
           of these two signals produces a third one with  vey line. Acquisition geometry very similar to
           a new frequency band, called a secondary fre-  this configuration is still used in marine explora-
           quency, which equals the difference between  tion and is known as single-channel seismic
           primary frequencies (f 3 ¼jf 1   f 2 j). For instance,  reflection. As its name indicates, seismic data
           using a primary frequency pair of 100 and    is collected using a very short streamer consist-
           104 kHz or 100 and 112 kHz, it is possible to  ing of only one single recording channel and a
           obtain 4 and 12 kHz secondary frequency sig-  single-channel seismic recorder. Although it is
           nals, respectively. Since a narrow secondary  supposed to be zero-offset acquisition, there is
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