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186   ZEOLITES AND MOLECULAR SIEVES

                     energy (see Eq. 7.1). For the same ion interacting with O 2 and N 2 ,the large
                     difference is caused by the difference in the quadrupole moment. The depen-
                     dence follows Eq. 7.3. In all cases, electrostatic interactions dominate (over the
                     dispersion forces).
                       In the example above, none of the adsorbate molecules are polar. The following
                     example illustrates interactions with polar molecules. Barrer and Gibbons (1965)
                     performed calculations on the interaction potentials of CO 2 and NH 3 moving
                     along the axis running through the center of the 12-ring window of the supercage
                     or central cavity of zeolite X. CO 2 has a strong quadrupole but no dipole, and
                     NH 3 has a strong permanent dipole but a weak quadrupole. The results are shown
                     in Tables 7.6 and 7.7. The qualitative comparison with experimental data was
                     remarkably good considering the calculations were made ca. 1965. In Table 7.6,
                     it is seen that the field gradient- quadrupole interaction dominates the adsorption
                     of CO 2 because it has no dipole but a strong quadrupole. The field gradient-
                     quadrupole interaction energy is nearly proportional to r −3  (Eq. 7.3), showing
                     the strong dependence on the ionic radius of the cation. For NH 3 , the field-dipole
                     interaction (φ Fµ ) is clearly important (Table 7.7). The φ Fµ term is proportional
                     to r −2  (Eq. 7.2), hence the φ Fµ term decreases sharply with increasing atomic
                     weight. The strong dependence on the cation size is also clearly seen for the
                     induction term, φ Ind (proportional to r −4 )(Table7.7).

                                 Table 7.6. Components of interaction energies (φ,in
                                 kJ/mol) for CO 2 adsorbed on X zeolite with different
                                 cations
                                 Component      Li +  Na +   K +  Rb +   Cs +

                                 −φ D (Oxygens)  15.9  13.0  7.1   4.6   4.6
                                 −φ D (Cations)  0.4   0.8   3.3   4.6   9.2
                                 −φ Ind          9.6   5.0   2.1   0.8   0
                                                30.9  21.3  17.6  14.6   9.6
                                 −φ ˙ FQ
                                 CO 2 is oriented along the ppp axis in the cavity (data taken
                                 from Barrer, 1978; Barrer and Gibbons, 1965). For CO 2 : µ = 0,
                                                            3
                                 Q =−4.3esu and α = 2.91 × 10 −24  cm /molecule.
                     Table 7.7. Energy terms in kJ/mol for NH 3 in X zeolite with different cations
                     Cation    −φ D       −φ D     −φ Fµ   −φ Ind   −φ total  Expt’L (− H)
                             (Oxygens)   (Cations)

                     Li +       47.2       1.7      50.6    23       77.7       76.5
                     Na +       33.8       3.3      33.0     9.6     53.9       72.3
                     K +         9.6       6.7      20.1     3.8     23.8       59.8
                     Rb +        7.9       11.7     17.6     2.9     20.5       55.6
                     Cs +        7.5       16.3     15.0     2.1     19.6       47.2
                     (Data taken from Barrer, 1978; Barrer and Gibbons, 1965). For NH 3 : µ = 1.47 debye, Q =−1.0
                                        3
                     esu and α = 2.2 × 10 −24  cm /molecule.
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