Page 153 - Fundamentals of Gas Shale Reservoirs
P. 153

WELL LOG ANALYSIS OF GAS SHALE RESERVOIRS  133
                  (a)                                          (b)
                       1                                            1

                      0.8                                          0.8


                    BI mineralogy  0.6          R  = 0.80        BI mineralogy  0.6            R  = 0.78

                                                                   0.4
                                                  2
                                                                                                2
                      0.4
                      0.2                                          0.2
                       0                                            0
                         0     0.2    0.4    0.6    0.8     1         0     0.2    0.4    0.6    0.8     1
                                                                                      BI
                                         BI sonic                                       sonic
            FIGURE 6.15  Cross‐plot analysis between BI mineralogy  and BI sonic  from two wells in Perth Basin, WA. BI mineralogy  calculated using mineralogy
            log data for well (a) and XRD analysis data for well (b).



            As is clear, this analysis requires full wave‐form sonic data,                    V –  V
            including shear wave and compressional wave velocities. In       Anisotropyindex x  sx  sy      (6.31)
            some cases, shear velocity is not available in the data set;                        V sx
            therefore, it should be estimated from the compressional
            velocity data. Using available  empirical formulas for the                        V – V
            shale layers like Castagna et al. (1985) formula, shear          Anisotropyindex   sx  sy       (6.32)
            velocity can be estimated as follows:                                          y    V sy

                           V   0 862  V  1 172         (6.30)    Finally, anisotropy of the formation can be calculated by tak­
                                .
                                         .
                            s         p
                                                                 ing a simple average from the anisotropy indices in X and Y
            where  V  and  V  are compressional and shear velocities   directions:
                   p
                          s
            respectively, in kilometers per second.
              Figure 6.15 shows the cross‐plot analysis between BI sonic    Averageanisotropy  Anisotropyindex  x  Anisotropyindex  y
            and BI mineralogy  using formula 6.1 for two wells in the Perth                     2
            Basin, WA. As (it is) expected, although there is a relatively                                  (6.33)
            good correlation coefficient between brittleness indexes
            from different methodologies, for both cases BI mineralogy  is
            higher than BI sonic . And as mentioned earlier, brittleness is   NOMENCLATURE
            a complex function of different parameters, not only miner­
            alogy; therefore, it seems that BI sonic  could give a better
            idea for determining prospect layers for doing hydraulic   a   Archie equation constant
            fracturing.                                          °C     Degree Celsius
                                                                 C      Stoichiometric constant relating kerogen to TOC in
                                                                  k
                                                                        Formula
            6.4.2.6  Determination  of Velocity  Anisotropy  Velocity
            anisotropy can take account of stratification, which is very   CO    Carbon dioxide
                                                                    2
            important for evaluating potential of the shale layers for   DT    Sonic transit time, μs/ft
            hydraulic fracturing. The relative anisotropy of the formation   DT     Fluid transit Time, μs/ft
                                                                   f
            could be computed by measuring the difference between   DT     Matrix transit Time, μs/ft
            shear wave velocity in X and Y directions (Tang et al., 2001).   DT ma  Kerogen transit time, μs/ft
            The difference between V  and V  can give an idea about the   E   TOC   Young’s modulus, Pa
                                sx
                                      sy
            relative anisotropy of the formation, which, for simplicity,
            could be called the anisotropy index. The anisotropy indices   G    Adsorbed gas capacity, scf/ton
                                                                  s
            in  X and  Y  directions are  calculated  by the following   K   Volume percent of kerogen, vol%
            formulas, respectively:                              m      Cementation exponent
   148   149   150   151   152   153   154   155   156   157   158