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In situ stress regimes with lithology-dependent and depletion effects  181


              constrained conditions than unconstrained conditions. The stress path order
              is as uniaxial strain > generalized plane strain > plane strain > uncon-
              strained. In their experiments a permanent stress change was also observed
              during the production and injection cycle for all boundary conditions. This
              indicates that most of stress changes during production are irrecoverable on
              repressurization. Therefore, decreasing depletion or slowing down pro-
              duction may reduce the irrecoverable reservoir damage.

              5.5.2 Depletion and Mohr’s circle representation
              The Mohr circle plots are useful for representing the depletion effect on the
              reservoir rock and for demonstrating how stress changes in the reservoir
              during its production history. As described in the previous section, the
              minimum horizontal stress decreases as the reservoir depletion increases.
              However, the vertical stress (overburden stress) does not change much
              (e.g., Segall and Fitzgerald, 1998); therefore, vertical effective stress increases
              as the depletion increases. Thus, a large stress difference in the effective
              vertical and minimum effective horizontal stresses is created as depletion
              increases, and the Mohr circle becomes larger. Fig. 5.13 presents the Mohr
              circles and the relationship of the minimum effective horizontal stress,
              effective vertical stress, shear stress, and the failure envelope for different
              degrees of depletion (Dohmen et al., 2017). Two cases are considered in the
              Mohr circle plots in Fig. 5.13 to allow for the uncertainty in Biot’s
              coefficient (i.e., a ¼ 0.5 and 0.75). Lower values of a, such as 0.3, shift the
              Mohr circles farther to the right (Fig. 5.13A), whereas higher values (e.g.,
              a > 0.75) shift the Mohr circles farther to the left (Fig. 5.13B), making the


              (A)                             (B)
                5000            Biot coeff = 0.5  5000           Biot coeff = 0.75
                     Mohr-Coulomb envelope 0.5  4000  Mohr-Coulomb envelope 0.5
               Shear stress (psi)  3000  No depletion  deple on  Shear stress (psi)  3000  No depletion  deple on
                4000
                     Depletion of 3000 psi
                                                      Depletion of 3000 psi
                                                      Depletion of 2000 psi
                     Depletion of 2000 psi
                                                2000
                2000
                1000
                 0                              1000 0
                  0    2000  4000  6000  8000  10000  0  2000  4000  6000  8000  10000
                            Effective stress (psi)           Effective stress (psi)
              Figure 5.13 Mohr circle representation showing the effects before (smallest circle) and
              after depletion of 2000 psi (intermediate circle) and 3000 psi (largest circle) in the
              Middle Bakken reservoir at the depth of 11,087 ft with the MohreCoulomb shear
              failure envelope (m ¼ 0.5) in a fractured formation (the line). (A) Biot’s coefficient
              a ¼ 0.5; (B) a ¼ 0.75.
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