Page 28 - Chemical equilibria Volume 4
P. 28

4     Chemical Equilibria
                           and:
                                 dn k  = ∑ ν ℜ                                           [1.4b]
                                 dt    ρ  k ρ  ρ
                             In these expressions,  dn  ,   ℜ and ν respectively denote the variation
                                                    k ρ  ρ      k ρ
                           of the quantity of the component A k due to the transformation ρ, the rate of
                           the transformation ρ  and the stoichiometric number relative to component
                           A k in the transformation ρ. The sum of relation [1.4b] is found for all of the
                           transformations taking place in the system under study.


                           1.2. Entropy production during the course of a transformation in
                           a closed system

                             Consider the transformation [1R.1]. We respectively denote by  d S  and
                                                                                        i
                           d S  the contributions to the entropy variation  made by the entropy
                            e
                           production within the system and the exchanges with the external medium.
                           The entropy balance at each moment can be written as:

                                 dS  =  d S  + d S                                        [1.5]
                                             e
                                       i
                                 dt    dt   dt
                             For our study, we choose as variables the p pertinent intensive variables
                           Y  and the quantities of material whose  fluxes are reduced, in a  closed
                            k
                           system, according  to relation [1.3], to the derivative of the extent of the
                           reaction. We can therefore express the entropy flux on the basis of those
                           variables, so:

                                       p
                                 d S  = ∑  S ∂  dY k  +  S ∂  dξ                          [1.6]
                                       1 Y
                                 dt   k= ∂  k  dt  ξ ∂  dt
                             In addition,  the entropy  contribution  due to the exchanges with the
                           external environment is linked to the exchanged heat, by:

                                 d S   1dQ
                                  e  =                                                    [1.7]
                                 dt    T  dt
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