Page 458 - Petrophysics
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426    PETROPHYSICS: RESERVOIR ROCK PROPERTIES
















                    Figure  7.3%  Carbonate rock  showing   Figure  7.3b. Carbonate rock  showing
                   pomsity:A,  vugs;  B,  joint  channels;   porosity  derived f?om  fracturing  and
                    C, bedding plane channels; 0, solution   fissuring [5].
                    cbanneZ [5J.
                    Fracture porosity is common in many sedimentary rocks and is formed
                    by structural failure of the rock under loads caused by various forms of
                    diastrophism, such as folding and faulting [8]. Solution or vuggy porosity
                    results from leaching of  carbonate rocks by circulating acidic waters.
                    Figures 7.3a and 7.3b show porosity derived from fracturing and fissuring,
                    and  porosity  derived from  solution along joints and  bedding planes,
                    respectively. Reservoir performance of most carbonates is considerably
                    different  than  that  of  sandstone  reservoirs  due  to  the  presence  of
                    strong  directional  permeability.  In  sandstone  reservoirs,  vertical
                    permeability, k,,  is generally much less than horizontal permeability, kn.
                    In contrast, k,,  in carbonate reservoirs commonly exceeds kh  due to the
                    dissolving effects of  hot  and acidic compaction-derived fluids moving
                    upward,  creating channels  and vugs  and  enlarging existing fractures
                    [7]. In sucrosic dolomite reservoirs with intergranular porosity, k,,  is
                    often approximately equal to kh.  Performance of  sucrosic dolomites
                    with  intergranular  interrhornbohedral  porosity  is  similar  to  that  of
                    sandstones [ 51.

             FLOW THROUGH FRACTURES

                      The significance of the fractures as fluid carriers can be evaluated by
                    considering a single fracture extending for some distance into the body
                    of  the rock and opening into the wellbore, as shown in Figure 7.4 [9].
                    Recalling the classical hydrodynamics equation for flow through slots
                    of fine clearances and unit width as reported by Croft and Kotyakhov
                    [lo, 111:

                         h3wfAp
                    q=  l2pL                                                     (7.31)


                    where:  h  = height (or thickness) of fracture, cm.
                           wf = width of fracture, cm.
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