Page 48 - Physical Principles of Sedimentary Basin Analysis
P. 48

30                        Properties of porous media

                 (b) The average permeability can be written as

                                                        k f w f
                                            k av = k 0 1 +                          (2.94)
                                                        k 0 w 0
                 which shows that the average permeability is much larger than the rock permeability k 0
                 when k f w f 
 k 0 w 0 .
                                                                             3
                 (c) The condition for fracture-dominated average permeability becomes w /12 
 k 0 w 0
                                                                             f
                 or w f 
 (12k 0 w 0 ) 1/3 .
                 (d) w 
 10 −5  m.
                 Exercise 2.20 Let a thin horizontal sheet of thickness h 1 be inserted into a layer of rock
                 with thickness h 0 . The sheet and the layer have the permeabilities k 1 and k 0 , respectively.
                 The sheet has a thickness that is much less than the layer (h 1 
 h 0 ).
                 (a) Show that the average vertical permeability of the composite layer is

                                   k 0 ,      h 1 /h 0 
 k 1 /k 0 ,  rock-dominated
                            k av =                                                  (2.95)
                                   k 1 (h 0 /h 1 ),  h 1 /h 0 
 k 1 /k 0 ,  sheet-dominated.
                 There are two regimes, one where the sheet does not alter the permeability of the block sig-
                 nificantly (rock-dominated), and another regime where the sheet controls the permeability
                 of the block (sheet-dominated).
                 (b) Assume that there is a pressure difference  p across the layer in the vertical direction.
                 Show that this pressure difference is almost entirely across the sheet when the average
                 permeability is sheet-dominated.
                 Solution:
                 (a) We have
                                               h 0 + h 1       k 0
                                     k av =               ≈         .               (2.96)
                                          (h 0 /k 0 ) + (h 1 /k 1 )  k 0 h 1
                                                            1 +
                                                                k 1 h 0
                 (b) The vertical Darcy flow through the layer is
                                             k av   p      k 1  p
                                         u =             ≈                          (2.97)
                                              μ (h 0 + h 1 )  μ h 1
                 when h 0 
 h 1 .


                 Exercise 2.21 A rectangular block is composed of two parts – one part of permeability
                 k 1 and thickness h 1 and another part of permeability k 2 and thickness h 2 , as shown by
                 Figure 2.19. The permeabilities parallel and normal to the layer are


                                                     k 1          h 1
                                                  k 2             h 2
                 Figure 2.19. A block is composed of two layers – one with permeability k 1 and thickness h 1 and
                 another of permeability k 2 and thickness h 2 . See Exercise 2.21.
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