Page 25 - Acquisition and Processing of Marine Seismic Data
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16                                    1. INTRODUCTION

           transmission. Each emitted beam is also per-  beams at both sides of the tow-fish. The maxi-
           ceived by the transducers during the recording,  mum recording distance is termed the sonar
           and forms an extremely high-amplitude input at  range. The distances are normally measured
           the zero time, called the output signal. Then the  along a slanted range from the transducers
           beams start to travel at both sides of the tow-fish  and do not correspond to horizontal distances,
           away from the transducers. The first meaningful  but can be converted into horizontal distances
           return is generally from the seafloor close to the  after a specific correction, termed the slant-
           tow-fish. Since the travel of the signal to and  range correction.
           from the seafloor will take some time, depend-  The returned signal to the sonar tow-fish is
           ing on the tow-fish altitude, and since almost  termed backscatter, notthe reflection, and is com-
           no signal amplitude is transmitted in a vertical  posed of backscattered energy because of the
           direction due to the directional pattern of the  roughness of the sediment particles on the sea-
           emitted signal, there will be a blank zone   floor. This roughness acts as a diffractor, which
           between the output signal and the seabed     scatters the energy in all directions, including
           return, which corresponds to the time span for  the tow-fish direction. Most of the emitted energy
           the sonar signal to travel through the water col-  from the transducers is reflected away from the
           umn to the seafloor and back to the tow-fish.  tow-fish direction, since the reflection angle
           This blank zone is indicated by the water col-  equals to the incidence angle. However, there
           umn in Fig. 1.10. Subsequent to this blank (and  will always be some amount of backscattered
           in most cases, amplitude free) zone, the seafloor  energy, which returns to the tow-fish, is per-
           return will arrive at the transducers. After that,  ceived by the transducers, and is recorded by
           returns from progressively distal ranges of the  the sonar recording unit. The amplitude of the
           seafloor are successively received by the trans-  backscatter is the main information received
           ducers. Returned amplitudes are recorded into  and recorded by the sonar system, and is used
           the disk files starting from time zero to the  to discriminate different types of seafloor sedi-
           end of the recording for both sides, after convert-  ments, since the backscatter amplitudes (in addi-
           ing their arrival time to one-way distance from  tion to the seafloor topography) are directly
           the tow-fish. Fig. 1.11 shows a sonar tow-fish  associated with the particle sizes (roughness)
           and a shallow water sonograph with small-scale  and composition of the seabed sediments. For
           boulders on a sandy seafloor.                instance, a common order of sediment roughness
              The beginning time of the recording, the time  from low to high may be clay, silty clay, silt, silty
           zero, is the time that the transducers emit the  sand, fine sand, and coarse sand. Therefore, each















           FIG. 1.11  (A) A sonar tow-fish and (B) a shallow water side-scan sonar record showing small-scale boulders on a sandy
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           seafloor. Sonar frequency is 455 kHz and the range is 50 m per side. Data is from Ozdaş, H., Kızıldag, N., Baydan, C., 2016. Ship-
           wreck Inventory Project of Turkey (SHIPT), Special Project Supported by Ministry of Development of Turkey.
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