Page 156 - Reservoir Geomechanics
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139    Rock failure in compression, tension and shear


                 Figure 4.31bagain illustrates the fact that elevated pore pressure reduces the differ-
               ence between principal stresses at depth as shown previously in Figure 4.30. When pore
               pressure is elevated, all three principal stresses are close in magnitude to the vertical
               stress and relatively small changes in the stress field can cause a transition from one
               style of faulting to another. Moos and Zoback (1993)hypothesize that because of ele-
               vated pore pressure at depth in the vicinity of Long Valley caldera, the style of faulting
               goes from NF/SS faulting on one side of the caldera to RF/SS faulting on the other side
               as the direction of the horizontal principal stresses change.
                 The stress polygon shown in Figure 4.31a permits a very wide range of stress values
               at depth and would not seem to be of much practical use in limiting stress magnitudes.
               However, as extended leak-off tests or hydraulic fracturing tests are often available to
               provide a good estimate of the least principal stress (Chapter 6), the polygon is useful
               for estimating the possible range of values of S Hmax .As noted above, we will illustrate in
               Chapters 7 and 8 that if one also has information about the existence of either compres-
               sive or tensile wellbore failures, one can often put relatively narrow (and hence, useful)
               bounds on possible stress states at depth. In other words, by combining the constraints
               on stress magnitudes obtained from the frictional strength of the crust, measurements
               of the least principal stress from leak-off tests and observations of wellbore failure
               place strong constraints on the in situ stress state (Chapters 6–8) which can be used
               to address the range of problems encountered in reservoir geomechanics addressed in
               Chapters 10–12.
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