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Formation Damage by Fines Migration: Mathematical and Laboratory Modeling, Field Cases  81


              and Born Repulsive potentials (Derjaguin and Landau, 1941; Elimelech
              et al., 2013; Gregory, 1981; Hogg et al., 1966; Israelachvili, 2011; Verwey
              et al., 1999).

                                  V 5 V LVW 1 V EDL 1 V BR ;              (3.9)
              where V is the total energy, V LVW is the London-Van der Waals potential,
              V EDL is the Electrical Double Layer potential, and V BR is the Born
              Repulsive potential.
                 The London-Van der Waals potential is the attraction between two
              closely separated surfaces and will mostly be attractive for the interaction
              between particles and grains in natural porous media. The force arises
              from the spontaneous electrical and magnetic polarizations, giving a
              fluctuating electromagnetic field within the medium. The classical
              approach to evaluating the London-Van der Waals interaction between
              two macroscopic bodies is obtained by pairwise summation of all the rele-
              vant intermolecular interactions. Retarded London-Van der Waals energy
              for sphere-plate interaction is given by the following formula (Gregory
              (1981)):

                                   A 132 r s  5:32h         λ w
                         V LVW 52         1 2      ln 1 1         ;      (3.10)
                                     6h        λ w        5:32h
              where A 132 is the Hamaker constant, λ w is the characteristic wavelength
              of interaction, and h is the surface-to-surface separation distance.
                 The expression for the Hamaker constant has the form (Israelachvili,
              2011):
                      3      ε 1 2 ε 3     ε 2 2 ε 3
                A 132 5 k B T
                      4      ε 1 1 ε 3  ε 2 1 ε 3
                                                                         (3.11)
                                            2   2     2  2
                                          n 2 n   n 2 n
                         3hv e             1    3  2    3
                      1 p  ffiffiffi                 n                     o ;
                                    1=2
                         8 2   n 1n 2      n 1 n 2     n 1n 2   1=2  1 n 1 n 2
                                                  2
                                        2
                                                              2

                               2
                               1  3     2    3    1   3       2    3
              where k B 5 1.381 3 10 223  J/K is Boltzmann constant, ε 1 , ε 2 ,and ε 3 are
              static dielectric constants of the particle, grain, and fluid, respectively, n 1 , n 2 ,
              and n 3 are the refractive indices of particle, grain, and fluid, respectively, and
                         15 21
              v e 5 3.0 3 10 s  is the constant value of absorption frequency.
                 The Born repulsive potential is a short-range repulsion that originates
              from the strong repulsive forces between the atoms as their electron shells
              interpenetrate each other. An expression for the Born repulsion potential
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