Page 77 - Adsorbents fundamentals and applications
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62   PORE SIZE DISTRIBUTION

                                         Sorbent  Adsorbate layer  Sorbent
                                         surface              surface
                                                     L

                                           d S                  d S














                                                       d A






                                              d 0           d 0
                                                   (L − d )
                                                       S
                                                  Free space
                     Figure 4.1. Single layer of adsorbate molecules in a slit-shaped adsorbent pore of width L
                     (Rege and Yang, 2000, with permission).



                     The average energy of a slit pore having 1 <M < 2is the same as ε 1 (z), since,
                     irrespective of M, the molecules are assumed to rest at a distance of d 0 from either
                     pore walls. The situation differs slightly when M ≥ 2. Three cases for this situa-
                     tion are depicted in Figures 4.2–4.4, wherein two different types of layers can be
                     visualized: the first type, consisting of the two layers in the immediate vicinity
                     of the two pore walls and at a distance of d 0 from them, and the second type of
                     molecules present in the interior of the pore sandwiched between two adjoining
                     adsorbate layers. The first type of molecules (marked A in the figure) will inter-
                     act with the sorbent molecules on one side and with adsorbate molecules on the
                     other. The distance between the two adsorbate molecules would be approximately
                     d A , using the same argument as discussed above. The interaction if energy of
                     this layer of molecules, denoted as ε 2 (z), is given by:

                                             4       10                  4        10


                               N S A S   σ S      σ S      N A A A    σ A     σ A
                        ε 2 (z) =  4  −       +          +    4   −        +
                                2σ       d 0      d 0       2σ        d A     d A
                                  S                           A
                                                                                   (4.20)
                     The second type of molecules (marked B in the figure), comprising (n − 2)
                     number of layers, will interact effectively only with two parallel planes of gas
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