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Seismic 2D Reflection Processing and Interpretation of ... - Posiva

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12Table 3. Example <strong>of</strong> a geometry file from the line 28. First 12 traces.TracenumberShotnumberGeophonenumberShotposition mGeophoneposition mCDPposition mOffset m1 1 1 -60 0 -30 602 1 2 -60 2,5 -28,75 62,53 1 3 -60 5 -27,5 654 1 4 -60 7,5 -26,25 67,55 1 5 -60 12,5 -23,75 72,56 1 6 -60 17,5 -21,25 77,57 1 7 -60 22,5 -18,75 82,58 1 8 -60 27,5 -16,25 87,59 1 9 -60 32,5 -13,75 92,510 1 10 -60 37,5 -11,25 97,511 1 11 -60 42,5 -8,75 102,512 1 12 -60 45 -7,5 105Geometric spreading correction (Table 2, item 4) was applied to seismic data by1,5multiplying amplitude data by t . Selection <strong>of</strong> parameter was based on a testing <strong>and</strong>references (Juhlin et al. 2004). Data was filtered (Table 2, item 5) using zero-phase,sine squared tapered b<strong>and</strong> pass filter (Stockwell & Cohen 2002) with the followingparameters.lower cut<strong>of</strong>f frequency: 30 Hzlower plateau frequency: 60 Hzupper plateau frequency: 400 Hzupper cut<strong>of</strong>f frequency: 600 HzPurpose <strong>of</strong> this preliminary filtering was to remove the highest <strong>and</strong> the lowestfrequencies. Selection <strong>of</strong> parameters was based on a raw spectrum. Example <strong>of</strong> aspectrum from the line S28 is shown in Figure 7. The frequency varies from very lowto very high frequencies. Shot gather after the preliminary filtering is shown in Figure8. Reflectors are not yet visible.

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