Page 28 - Adsorbents fundamentals and applications
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BASIC CONSIDERATIONS FOR SORBENT DESIGN  13

                        Table 2.2. Polarizabilities (α) of ground state atoms and
                                    3
                        ions (in 10 −24  cm )
                        Atom     α     Atom      α     Atom     α

                        C       1.76   K       43.4    Co      7.5
                        N       1.10   Rb      47.3    Ni      6.8
                        O       0.802  Cs      59.6
                        F       0.557  Mg      10.6    Li +    0.029
                        S       2.90   Ca      22.8    Na +    0.180
                        Cl      2.18   Sr      27.6    K +     0.840
                        Br      3.05   Ba      39.7    Ca 2+   0.471
                        I       5.35   Al       6.8    Sr 2+   0.863
                                       Si       5.38   Ba 2+   1.560
                        Li     24.3    Fe       8.4
                        Na     24.08


            selected atoms are given in Table 2.2. It can be seen that the alkali and alkaline
            earth metal atoms have very high polarizabilities. Hence these elements, when
            present on the surface, can cause high dispersion potentials. When these elements
            are present as cations, however, the polarizabilities are drastically reduced. The
            polarizabilities of selected cations are also included in Table 2.2 for comparison.
              For electrostatic interactions, the charges (q) and the van der Waals radii of the
            surface atoms (or ions) are most important. For ionic solids with point charges dis-
            tributed on the surface, the positive and negative fields can partially offset when
            spaced closely. However, anions are normally bigger than cations. Consequently,
            the surface has a negative electric field. All electrostatic interaction potentials are
                                            2
                                       ) or q (  Ind ) and are inversely proportional to
            proportional to q(  Fµ and   ˙ FQ
             n
            r (where n = 2–4, see Eqs. 2–8). Here, r is the distance between the centers of
            the interacting pair, which should be the sum of the van der Waals radii of the two
            interacting atoms. Hence, the van der Waals radii of the ions on the surface are
            important. The strong effects of charge (q) and ionic radius of the cation on the
            adsorption properties of ion-exchanged zeolites will be discussed in Chapter 7.
              Because the ionic radius determines the distance r, it has a strong effect on the
            electrostatic interactions. The ionic radii of selected cations are given in Table 2.3.
            The ionic radius is a crucially important factor when considering ion-exchanged
            zeolites and molecular sieves as sorbents.

            2.4.2. Pore Size and Geometry
            The potentials discussed above are those between two molecules/atoms. The
            interactions between a molecule and a flat solid surface are greater because the
            molecule interacts with all adjacent atoms on the surface, and these interac-
            tions are assumed pairwise additive. When a molecule is placed between two
            flat surfaces, i.e., in a slit-shaped pore, it interacts with both surfaces, and the
            potentials on the two surfaces overlap. The extent of the overlap depends on
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