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EQUILIBRIUM ISOTHERMS AND DIFFUSION  21

            where
                                              RT
                                         C =                              (3.10)
                                              βE 0
            where E 0 is the characteristic energy of adsorption of a standard vapor (usually
            benzene). A theoretical basis has been given for the D–R equation (Chen and
            Yang, 1994), by a simple statistical mechanical derivation assuming a mean field
            that is related to the characteristic energy and some simplifying manipulations.
            This mean field was later related to the pore dimension and other properties
            (Chen and Yang, 1996; Hutson and Yang, 1997).
              The exponent “2” in the D–R equation can be replaced by n, which is called
            the Dubinin–Astakhov equation (or D–A equation). The value of n empirically
            ranges from below 1 to about 14 (Kapoor and Yang, 1988; Kapoor et al., 1989a).
            The parameter n can be related to heterogeneity (Jaroniec and Madey, 1988;
            Rudzinski and Everett, 1992). The theoretical basis given by Chen and Yang
            (1994) is also valid for the D–A equation.
              The potential theory isotherm can be extended to adsorption of mixed gases,
            as done by Bering et al. (1963 and 1965), and reviewed in Yang (1987). The
            model by Grant and Manes (1966) has been discussed in detail by Yang (1987).
            A simple and explicit model has been proposed by Doong and Yang (1988),
            which is given below. Doong and Yang (1988) extended the D–R equation to
            mixed-gas adsorption in a simple way by using the concept of maximum available
            pore volume without any additional equations such as the Lewis relationship (see
            Yang, 1987). For binary mixtures:

                                                            2


                                                       P 01
                             V 1 = (V 01 − V 2 ) exp − C 1 ln             (3.11)
                                                        P 1
                                                            2


                                                       P 02
                             V 2 = (V 02 − V 1 ) exp − C 2 ln             (3.12)
                                                        P 2
              In Eq. 3.11, V 01 is the limiting pore volume for component 1 and V 2 is the
            actual adsorbed amount for component 2. All parameters that characterize the
            gas-sorbent system for the single gases remain unchanged for the mixture. The
            two equations can be solved easily. This model can be readily extended to mul-
            ticomponent mixtures. This model has been applied favorably for fitting experi-
            mental data (Doong and Yang, 1988). It has been used recently for the adsorption
            of mixtures of CO 2 /H 2 O on NaX zeolite and γ -alumina (Rege and Yang, 2001a),
            and it compared favorably against the ideal adsorbed solution theory. The D–A
            equation can be extended in the same manner as the D–R equation, by retaining
            the individual exponent (n i ) for each component (Takahashi et al., 2001).
              Wood (2002) has recently made an extensive comparison of different models
            for predicting mixture adsorption from single-component D–R isotherms. The
            data of a total of 93 binary mixtures of organic vapors on activated carbon were
            compared. Despite the simplicity of the model (Eqs. 3.11 and 3.12), predictions
            were among the best.
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