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22   SORBENT SELECTION: CRITERIA

                     3.1.3. Ideal Adsorbed Solution Theory for Mixture and Similarities
                     with Langmuir and Potential Theories

                     The ideal adsorbed solution (IAS) theory of Myers and Prausnitz (1965) was
                     the first major theory for predicting mixed gas adsorption from pure component
                     isotherms, and it remains the most widely accepted. There have been approxi-
                     mately a dozen other theories that have been discussed in Yang (1987); however,
                     they are not repeated here.
                       The adsorbed mixture is treated as a two-dimensional phase. From the Gibbs
                     isotherm, one can calculate a spreading pressure for each component based on
                     its pure component isotherm. The basic assumption of the IAS theory is that the
                     spreading pressures are equal for all components at equilibrium.
                       The spreading pressure, π, is given by:

                                               πA       P  q
                                                   =       dP                      (3.13)
                                               RT     0  P

                     where q is related to P by any pure component isotherm. Assuming the activity
                     coefficients are unity for all components in the adsorbed mixture, the IAS model
                     consists of the following set of equations, for a two-component mixture:

                                               P  0        P  0
                                               1 q 1       2 q 2
                                                  dP =        dP                   (3.14)
                                                P           P
                                             0           0
                     The Raoult’s law, or Eq. 3.15, is written for both species:
                                                  0
                                          PY 1 = P X 1                             (3.15)
                                                  1
                                                  0
                                                          0
                                          PY 2 = P X 2 = P (1 − X 1 )              (3.16)
                                                  2
                                                          2
                            0
                     where P is the equilibrium “vapor pressure” for pure i adsorption at the same
                            i
                     spreading pressure, π,and the same T as the adsorbed mixture. These three
                     equations (Eqs. 3.14, 3.15, and 3.16) define the adsorbed mixture. For example,
                     if P and Y 1 (and Y 2 ) are given (T is already given), the three equations are solved
                         0
                             0
                     for P , P ,and X 1 . Equation 3.14 can be integrated to yield an algebraic equation
                         1  2
                     if the isotherms have certain forms like Langmuir and Freundlich equations.
                                                                            0   0
                     Otherwise, Eq. 3.14 is solved numerically. With the values of P , P ,and X 1
                                                                           1   2
                     determined, the following equations are used to calculate q 1 , q 2 ,and q t :
                                            1     X 1      X 2
                                              =      0  +    0                     (3.17)
                                                q 1 (P )  q 2 (P )
                                            q t
                                                    1        2
                                                                                   (3.18)
                                            q 1 = q t X 1 and q 2 = q t X 2
                       For systems following the Langmuir isotherm, the IAS theory is identical to
                     the extended Langmuir equation for mixtures, if the saturated amounts are equal
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