Page 166 - Book Hosokawa Nanoparticle Technology Handbook
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FUNDAMENTALS                CH. 3 CHARACTERISTICS AND BEHAVIOR OF NANOPARTICLES AND ITS DISPERSION SYSTEMS

                                        V     V B



                                                V R

                                             V T
                                         0
                                                                                ( r 2−  a)  a /
                                                                   Secondary minimum
                                                V A




                                                  Primary
                                                             (a)
                                                  minimum

                                                                    V B
                                   V B
                                               -3
                              V           C e = 10 mol/l       V           = 65 mV
                                                                          0
                                               -2
                                             10 mol/l                       50 mV
                                               -1
                                             10 mol/l                       35 mV
                              0                                 0
                                                                                          −
                                                        −
                                                      ( r 2 a)  a /                     ( r 2 a)  a /
                                                                       V A (  = 0 mV)
                                                                           0
                                   V A
                                                                                -2
                                              = 65 mV                      C e = 10 mol/l
                                             0
                                               (b)                              (c)
                  Figure 3.5.11
                  Typical interaction potentials V between charged particles in solutions given by DLVO theory (a), the dependence on the
                  electrolyte concentration (b), and the dependence on the surface potential (c).
                    3.5.2.3 Control of dispersion stability using DLVO theory  where the temperature and Hamaker constant are
                  As known from equations (3.5.50) and (3.5.52), the  given by T(K) and A(J), respectively. This indicates
                  variable parameters in these equations are   and C e  that the value of CCC for trivalent cations is 1/729 of
                                                      0
                  (or  ) only, because the others belong to the specific  CCC value for mono-valent cations. This dependence
                  properties of dispersions.  The value of  C may be  of  CCC on  z is confirmed experimentally, and the
                                                     e
                  altered by adding salts, and that of   by the solution  relation is known as the Schulze–Hardy law.  This
                                                0
                  pH.  As illustrated in Fig. 2(b), (c), the dispersion  coincidence between the prediction by the DLVO
                  becomes unstable, as C increases or   decreases.  theory and experimental results is one of the reasons
                                     e
                                                 0
                    When the value of  C increases, the electrostatic  why the DLVO theory has been widely accepted as
                                      e
                  repulsive potential disappears and the potential nearly  the fundamental theory for hydrophobic colloids. In
                  coincides with the van der Waals potential at the so-  the many real colloids, the following relation may
                  called critical coagulation concentration (CCC). At  be used.
                  C   CCC, the coagulation rate becomes constant. This
                   e
                  region is called the rapid coagulation region, and that of  CCC
   z   n  ( n   2 	  ) 6  (3.5.55)
                  C   CCC is called the slow coagulation region. It is
                   e
                  known that the value of CCC depends on z. According  This rule indicates that stable dispersions are obtain-
                  to the theoretical prediction, CCC(mol/l) for particles of  able by reducing the concentration of multi-valent
                  high surface potential is expressed by the following  ions, while the addition of multi-valent ions is very
                  equation:                                      effective to promote the coagulation and the
                                                                 solid–liquid separation. The stability of dispersions is


                                             5
                                                 2
                                               6
                            CCC  72  10  57 3 T z A          (3.5.54)  controllable also by the surface potential   . At the
                                   .
                                           r                                                        0
                  142
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