Page 278 - Reservoir Geomechanics
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259    Wellbore failure and stress determination in deviated wells



        a.                                        b.

                       Plane normal                              Plane normal
                       to borehole                               to borehole







                               Fast
                                                                         Fast
                                 Fast                                   Fast










              Figure 8.16. (a) Geometry of a borehole at an oblique angle to a vertically transverse formation and
              (b) the general case when a borehole is oblique to a formation with a symmetry axis that is not
              aligned with one of the cartesian coordinate axes. After Boness and Zoback (2006).



              avertical pilot holedrilled to2.2kmdepthingranodioriteandawelldeviated ∼55 from
                                                                                 ◦
              vertical below 1.5 km depth that encountered an alternating sequence of sedimentary
              rocks below 1920 m depth (measured depth). Independent data are available on the
              orientations of bedding planes and fractures from electrical imaging data as well as
              breakouts and drilling-induced tensile fractures in the vertical pilot hole (Hickman and
              Zoback 2004). Boness and Zoback (2004) showed that in the vertical pilot hole, the fast
              shear velocity anisotropy direction was parallel to the direction of maximum horizontal
              compression obtained from wellbore failures apparently caused by the preferential
              closure of fractures in response to an anisotropic stress state.
                Figure 8.17 (from Boness and Zoback 2006) illustrates the three-dimensional model
              for computing the apparent fast direction that will be recorded on the dipole sonic tools
              for any arbitrary orientation of the borehole and dipping bedding planes. In the case of
              stress-induced anisotropy, the true fast direction is parallel to the maximum compressive
              stress, oriented across the closed fractures. Thus, the apparent fast direction is not
              described by a plane but rather a line that lies within the plane normal to the borehole,
              in the direction normal to the fracture opening direction. The apparent fast direction is
              the vertical projection of the maximum compressive stress on the plane perpendicular
              to the borehole and will have the same azimuth as S Hmax (Figure 8.17b), with a dip that
              depends on the orientation of the borehole. In the case of structural anisotropy, the true
              fast direction is oriented along the planes (be they fractures/bedding/aligned minerals)
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