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100   Applied Petroleum Geomechanics


          3.2.2 Empirical equations of rock strengths in sandstones
          3.2.2.1 From sonic velocity and transit time
          For fine grained, both consolidated and unconsolidated sandstones in the
          Bowen Basin of Australia, McNally (1987) presented the following strength
          estimation using sonic logs:

                              UCS ¼ 1200 expð 0:036DtÞ                (3.17)
          where UCS is in MPa and the transit time Dt is in ms/ft.
             For the Tertiary reservoir sandstones in the Gulf of Mexico and the
          Jurassic reservoir sandstones in the North Sea, the following correlation
          exists between the lab-measured UCS and the compressional transit time
          from sonic log measurements (Fig. 3.12):
                                                   2:064
                               UCS ¼ 156318ð1=DtÞ                     (3.18)





















          Figure 3.12 Lab-measured uniaxial compressive strengths versus sonic compressional
          transit time in some deep wells in the Gulf of Mexico and the North Sea.



             The same units are used as those in Eq. (3.17).
             Some high-porosity (w20%) sandstones are even weaker than shales,
          such as the Tertiary formations in the Gulf of Mexico. In this case, the
          wellbore breakout and sand production are expected while drilling and
          after reservoir production. Based on the laboratory test data in the Tertiary
          formations of the Gulf of Mexico and the North Sea, Zhang (2013) ob-
          tained the following empirical equation to estimate the UCS for weak
          (poorly consolidated) sandstones:

                                                    2:5
                               UCS ¼ 0:68ð304:8=DtÞ                   (3.19)
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