2 Thermodynamics Framework
From the formalism of the classical thermodynamics [12] entropy
production can be evaluated through the variation of Gibbs’s free
energydGTpwhen the system evolves subjected to the constraints
the temperatureTand the pressurepconstants as
δSi¼
1
T
dGTp ð 1 Þ
The temporal variation of the expression of Eq. (1) represents
the entropy production rate as
δSi
dt
¼
1
T
dGTp
dt
ð 2 Þ
whereδdtSiS_irepresents the entropy production rate. The termdGdtTp
can be developed by means of the chain rule as a function of the
degree of advance of the reactionξas
dGTp
dt
¼
∂G
∂ξ
Tp
dξ
dt
ð 3 Þ
where ∂∂Gξ
Tp
, according to De Donder and Van Rysselberghe
[13],represents the affinityA¼∂∂Gξ
Tp
, and the termddtξis the
reaction rateξ_.
The rate of entropy production (Eq.3) can be written as
δSi
∂t
¼S_i¼
1
T
Aξ_¼
1
T
ΔG_ξ ð 4 Þ
whereA¼ΔG. The affinityAcan be evaluated from the iso-
therm of the reaction [14] by the equation
A¼RTlnKCRT
Xk
i¼ 1
νklnCk¼RTln
KC
∏Cνkk
ð 5 Þ
where KC¼kkbf is the Guldberg-Waage constant;kf,kbare the
specific rate constants of the direct and inverse reaction stepsf,b,
respectively;Ckis the concentration of thekth specie; and theνkare
the stoichiometric coefficients that are taken, by agreement, as
positive for the products and negative for the reactants. Therefore,
Eq. (5) can be written as
A¼RTln
kf∏C
νkfðÞ
kfðÞ
kb∏C
νkbðÞ
kbðÞ
!
ð 6 Þ
The rate of reactionξ_can be written as
ξ_¼ ξ_fξ_b
¼kf∏C
νkfðÞ
kfðÞkb∏C
νkbðÞ
kbðÞ ð^7 Þ
130 Sheyla Montero et al.