Page 495 - Acquisition and Processing of Marine Seismic Data
P. 495

486                      10. NORMAL MOVEOUT CORRECTION AND STACKING



































           FIG. 10.28  A comparison of (A) conventional NMO/stack, and (B) CRS stack sections. Data quality is significantly
           improved in the CRS stack, especially for the reflections at the central part where a thrust fault is observed.


              10.5 QC IN NMO CORRECTION                    In Fig. 10.29A, a number of NMO corrected
                       AND STACKING                     consecutive CDPs are displayed for QC pur-
                                                        poses. In areas indicated by blue polygons, the
              One of the most important QC applications  reflections are not flattened at all, due to the
           for NMO correction is to display and check the  fact that the velocities used for NMO correction
           NMO corrected CDPs to ensure that all of the  are too fast for polygon A, while they are too
           primary events are flattened, which is the ulti-  slow for polygon B. Turning back to the velocity
           mate goal of the NMO correction. Since the suc-  analysis, the velocity picks for the CDPs in the
           cess of the correction directly depends on the  polygonal areas must be corrected and updated,
           correctness of the velocity function used, veloc-  as shown in Fig. 10.29B. If not, the reflections
           ity picks around the problematic CDPs after  that are not perfectly flattened cause severe
           NMO correction must be edited to obtain a more  degradations on the stacked trace. Fig. 10.30
           accurate velocity function, which flattens the  shows this effect on a synthetic CDP with two
           primary reflections. Apart from improper veloc-  reflection hyperbolas. If we use accurate veloci-
           ity functions used, unflattening frequently  ties for both reflections in NMO correction (e.g.,
           occurs in areas of steep dip and complex seafloor  V 1 ¼ 1500 m/s and V 2 ¼ 1800 m/s for shallow
           morphology, where the reflections may not be  and deep reflections, respectively), we get per-
           hyperbolic.                                  fectly flattened hyperbolas with a favorable
   490   491   492   493   494   495   496   497   498   499   500