Page 14 - Partition & Adsorption of Organic Contaminants in Environmental Systems
P. 14

SECOND LAW OF THERMODYNAMICS       5

            becomes the criterion for any infinitesimal process within a closed system (i.e.,
            where no mass transfer occurs across the system boundary) to take place at
            equilibrium [i.e., (dG) T,P = 0] or spontaneously [i.e., (dG) T,P < 0] at constant
            temperature and pressure. For a single-component system, dG is a function of
            temperature and pressure (or volume). For a complex mixture, dG depends
            also on the composition, as will be seen.
              If a phase transition (e.g., from liquid to vapor) takes place in a closed
            single-component system at constant  T and  P, the transition can thus be
            carried out at equilibrium with any phase-mass ratio as long as both phases
            coexist in finite amounts. In this case, dG/dl, or DG, is equal to 0, where DG
            corresponds to a finite phase transition and l is the progress variable. In a
            closed multicomponent system where a chemical reaction takes place or a
            component distributes between phases at fixed T and P, usually only one com-
            position can satisfy the condition for equilibrium (i.e., dG/dl=DG = 0).
              For simple systems without mass and composition changes, one can thus
            write

                                      dE =  T dS -  P dV                   (1.8)

            and

                                                      -
                                                +
                                         +
                                                           -
                                   -
                             =
                          dG T dS P dV P dV V dP T dS SdT
            or
                                      dG =  V dP -  S dT                  (1.15)
              In a closed system where a change in state or a chemical reaction takes
            place at constant temperature, one finds from Eq. (1.12) an important relation
            as follows:

                                      DG =  DH T  DS                      (1.16)
                                               -
            Thus, the reduction in free energy of a closed system at constant temperature
            is favored by a decrease in system enthalpy or by an increase in system
            entropy. However, chemical processes seldom occur with emission of heat (i.e.,
            DH < 0) coupled with an increase in DS. In some special cases, the process may
            proceed with DH = 0 and TDS > 0, such as the expansion and mixing of ideal
            gases or the formation of an ideal solution, or with DH < 0 and TDS   0, such
            as chemical reactions in which the moles of reactants equal the moles of prod-
            ucts. Frequently, chemical processes occur with opposing effects of DH and T
            DS, in which one outweighs the other.
              To illustrate how either DH or TDS may act as the main driving force for a
            spontaneous process, let us consider two physical processes, vaporization and
            adsorption, at constant temperature in a closed system. When a fraction of a
            liquid in excess quantity is being evaporated into a fixed vacuum space, the
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