Page 104 - Adsorption by Powders and Porous Solids
P. 104

CHAPTER 3. METHODOLOGY OF ADS0Rpirlo~

              Table 3.1.  Thermal transpiration: coefticients of the Takaishi and
              Sensui equation, for various gases.
              Gas         A    B      C     Temperature range (K)
              Hydrogen
              Neon
              Argon
              Krypton
              Methane
              Xenon
              Helium
              Nitrogen
              oxygen




    3.4.8.  Correction for non-ideality
    At the temperatures normally used for physical adsorption, the correction for the non-
    ideality of real gases generally amounts to several percent. It can be reasonably taken
    into account by using the first two terms of the virial equation:




    where u",  and vyd are the real and ideal molar volumes of the gas at a given temper-
    me T and reference pressure (normally 1 bar), respectively, V is the total volume
    occupied by the given amount of gas, and B,  is the second molar virial coefficient,
    which  is usually  negative under the  conditions of  physisorption experiments. Its
    value for a large number of gases can be found in a critical compilation by Dymond
    and Smith (1969) and in the thermodynamic tables published by Marsh (1985).
     To determine the real amount of gas present in a given volume V, at temperature T
    and pressure p, it is convenient to use the relation:




    where  V  is  expressed  in  cm3  and  p  in  bar  and  where  a=-100B,/~~~=
    -(IoB,,,/RT) xpO.
     Values of a for a number of gases and temperatures used in adsorption studies are
    given in Table 3.2. They were calculated with help of the data provided by Dymond
    and  Smith (1969). A  detailed study of  the  incidence of  these corrections on the
    adsorption isotherms and the BET surface areas was made by Jelinek et al. (1990).
     An elegant way to avoid this non-ideality correction, especially when operating at
    high pressures (up to 16.5 MPa), where it can become predominant, was proposed by
    Bose et al. (1987). In  their method, for each equilibrium point the density of  the
    adsorptive is determined experimentally from its dielectric constant, which is mea-
    sured in a gas capacitance cell at the same temperature and pressure as the adsorption
    system  studied.  The  rest  of  their  adsorption  procedure  is  comparable  to  the
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