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stretched by 1.6m. From rock physics it is well known that such stretching will reduce the P-wave velocity of the rock, and hence will introduce an overburden time shift. Guilbot and Smith (2002) used


4D traveltime shifts to conclude that the overburden at Ekofisk had been stretched and that the chalk reservoir rock was compacted due to production. A 4D traveltime shift means that the traveltime between two seismic horizons (representing geological interfaces in the subsurface) has changed. Guilbot and Smith found that the time shift for the overburden was up to 18 ms between 1989 and 1999. Te overburden thickness at Ekofisk is approximately 3 km. Tis time shift was positive, meaning that the average P-wave velocity in the overburden had decreased between 1989 and 1999. For the same period they found a negative time shift of up to 10 ms for the Ekofisk reservoir formation, which was not a huge surprise since it was well known that the seafloor at Ekofisk had undergone severe subsidence. Te compaction of the reservoir was also well known, and it was understood as well that the subsidence was less than the compaction at reservoir level, and hence the overburden had been stretched. What was new and exciting in Guilbot and Smith’s findings was that time-lapse seismic could be used to quantify compaction and thus to create maps that show that some reservoir compartments are more compacted than others. Tis initiated new research on how to couple geomechanical modelling with time-lapse seismic measurements.


1250m


N 2/4-X-27 2/4-X-09


N


1250m


Figure 4.21: 4D time shifts for top reservoir interface (left) and for the Ekofisk Formation (right). The black area in the middle is caused by the gas chimney problem at Ekofisk, leading to lack of high quality seismic data in this area. Notice that some areas of the reservoir zone (right) are more compacted than others.


4.2.1 Reservoir Compaction and Velocity Changes


When the reservoir rock compacts, the over- and underburden are stretched. Tis stretch is relatively small (of the order of 0.05%). However, it produces a small velocity decrease that is observable as time shifts on time-lapse seismic data. A simple calculation can help us to understand why time-


lapse seismic can detect such small changes. Assume that the velocity decrease caused by the stretching of the overburden is -0.1%. As an example we can assume that the average


167


Time (ms TWT)


Time (ms TWT)


Guilbot and Smith, TLE, 2002


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