Page 283 - Acquisition and Processing of Marine Seismic Data
P. 283

274                                   5. PREPROCESSING


































           FIG. 5.33  Schematic illustration of the attenuation effect on a sine wave. (A) Input monofrequency sinusoid, after
           (B) spherical divergence and (C) absorption effects. T and A represent period and amplitude of the sinusoid, respectively.
           Only amplitude decay occurs in the case of the spherical divergence effect, while both amplitude decay and frequency
           decrease occur due to the absorption effect. Here, T 1 ¼ T 2 < T 3 and A 1 > A 2 > A 3 .

                                    e  αr               absorb the signal quickly, and this causes serious
                          ArðÞ ¼ A 0ðÞ            (5.6)
                                     r                  issues in land seismic surveys because the surfi-
                                                        cial weathered soil layer does not only absorb the
           Eq. (5.6) suggests several implications: first,  signal, but also creates lateral velocity variations.
           higher frequency components are absorbed     To overcome this issue, dynamite is located into
           more quickly with respect to the lower fre-  the shallow bore holes penetrating the base of the
           quency components of the signal. Therefore,  surficial weathered layer.
           higher frequency amplitudes of the propagating  Although fluid saturation and free gas con-
           signal die rapidly, the period (and hence the  tent of the pore spaces contribute to absorption,
           wavelength) of the signal increases and the dom-  the primary reason is the transformation of the
           inant frequency decreases. In addition, the  kinetic energy into heat energy due to the fric-
           absorption of the signal becomes higher as the  tion of the rock particles during the wave pas-
           absorption coefficient increases. For a constant  sage.  The  heat  emerging  during  the
           velocity subsurface, the absorption coefficient  compression when the acoustic wave travels
           of the medium is mainly controlled by the rock  through a medium is consumed during the dila-
           quality factor, Q, which has a relatively small  tation and cannot be recovered. The longer the
           value for weathered layers while it is larger for  signal travels, the higher the effect of the absorp-
           massive and compact media. Weathered layers  tion is, and therefore reflections from deeper
   278   279   280   281   282   283   284   285   286   287   288