Page 85 - Applied Petroleum Geomechanics
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76    Applied Petroleum Geomechanics


             It is rarely reported on how to convert dynamic Biot’scoefficient to
          the static one. However, dynamic bulk modulus can be related to static
          bulk modulus by using empirical equations presented in Section 2.5.5.
          As described in Section 2.6.3, the difference of dynamic and static
          Poisson’s ratios is small; therefore, the correlations of dynamic and static
          Young’s moduli can be used to obtain the correlations in dynamic and
          static bulk moduli. For example, Eq. (2.72) can be expressed in the
          following form:

                                      K s ¼ kK d                      (2.82)
          where K s and K d are the static and dynamic bulk moduli, respectively; k is a
          correlation factor between 0.5 and 0.79 from Eq. (2.72).
             Combining Eqs. (2.81) and (2.82), the static Biot’s coefficient, a, can be
          obtained in the following form:

                                      kr V   4V   sd 2    3
                                            2
                                        d
                                            pd
                              a ¼ 1                                   (2.83)
                                             K m
          where k is a correlation factor between 0.5 and 0.79 from Eq. (2.72).
             Combining Eqs. (2.83) and (2.81), the relation of dynamic and static
          Biot’s coefficients can be obtained, i.e.,

                                  a ¼ð1   kÞþ ka d                    (2.84)
             For example, if a d ¼ 0.7 and k ¼ 0.6, then from Eq. (2.84) a ¼ 0.82.
             Fabricius et al. (2008) studied dynamic Biot’s coefficients in the North
          Sea chalk samples, which varied considerably in depositional texture and
          mineralogy. They calculated dynamic Biot’s coefficients from Eq. (2.81)
          using the velocities of the dry chalk samples and the matrix bulk modulus of
          calcite. Their results indicate that dynamic Biot’s coefficient tends to
          decrease with porosity in clay-poor samples as a reflection of calcite
          cementation, causing the mineral frame to stiffen as porosity is filled by
          cement. Samples rich in smectite or chlorite tend to have relatively high
          Biot’s coefficient, probably because the presence of clay prevents calcite
          cement from bridging between particles.

          2.7.3 Empirical methods for Biot’s coefficient
          If no measured Biot’s coefficient is available, the empirical equations can be
          used to estimate Biot’s coefficient. Experimental results show that Biot’s
          coefficient is a function of porosity; therefore, most empirical equations for
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