Page 27 - Chemical equilibria Volume 4
P. 27

Physico-Chemical Transformations and Equilibria     3
                             Thus, we speak of the enthalpy, Gibbs energy, entropy, variations in
                           volume, etc. associated with the transformation.
                           1.1.3. Standard values associated with a transformation

                             We shall see that in the particular case where we choose pure components
                           in their phases, at a pressure of 1 bar, the standard value A associated with
                           the reaction [1R.1] is defined by the relation:

                                 Δ A = ∑ ν i i o                                          [1.2]
                                    0
                                           a
                                  r
                                        i
                               o
                              a  is the standard value of the parameter A of the i, meaning that the
                               i
                           value of A taken in the pure state at a pressure of 1 bar at the temperature of
                           298 K (25ºC), the substance being in its normal state of condensation at that
                           temperature and pressure. We thus define a standard value at temperature T
                           as the above standard value chosen at the temperature T instead of 298 K.


                           1.1.4. Extent and rate of a transformation

                             A transformation is also characterized by its extent  ξ  at a time t and its
                           rate  ℜ  at that instant. The rate is the derivative in relation to time of the
                           extent. If n k is the number of moles of the component A k, we have:
                                 dξ =  1  dn k                                           [1.3a]
                                 dt  ν k  dt


                           and:

                                     dξ
                                 ℜ=                                                      [1.3b]
                                     dt

                             In the case where  multiple transformations take place in the system,
                           equations [1.3a] and [1.3b] are replaced by:

                                 dn
                                   k ρ  = ν ℜ                                            [1.4a]
                                  dt    k ρ  ρ
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