Model-Based Analysis: Reaction Types

The rate of chemical reaction for each individual reaction step j can be written as the product of two functions, where the first function fj(ej,pj) depends on the concentrations of reactant (ej) and product (pj). (see also Model-Based: General). The second function Kj(T) depends on temperature.

For all chemical reactions the Arrhenius temperature dependence with activation energy Ej is used:

Kj(T)=exp[-Ej/(RT)]

The dependence on concentrations f(e,p) can be described by the following reaction types (only first elements are shown, use scroll bar to view the rest):

Code Function Type of Reaction
F1 f = e Reaction of 1st order
F2 f = e2 Reaction of 2nd order
Fn f = en Reaction of nth order
FnR Reversible reaction of nth order
R2 f = 2e1/2 Two-dimensional phase boundary
R3 f = 3e2/3 Three-dimensional phase boundary
D1 f = 0.5 / p One-dimensional diffusion
DFn f = en · 0.5 / p One-dimensional diffusion with n-th order
D2 f = -1 / ln(e) Two-dimensional diffusion
D3 f = 1.5e2/3 / (1 - e1/3) Three-dimensional diffusion Jander’s type
D4 f = 1.5 / (e-1/3 – 1) Three-dimensional diffusion Ginstling-Brounstein type
B1 f = e·p  Prout-Tompkins equation
Bna f = en·pAutocatOrder  Expanded Prout-Tompkins equation
SB f = en·pm · [-ln(e)]q Expanded Sestak-Berggren equation
C1 f = e·(1 + AutocatPreExp · p) Reaction of 1st order with autocatalysis by product
Cn f = en·(1 + AutocatPreExp · p) Reaction of nthorder with autocatalysis by product
Cnm f = en·(1 + AutocatPreExp · pm) Reaction of nth order with m-Power autocatalysis by product
Kamal-Sourour*    
A2 f = 2e·[-ln(e)]1/2  Two-dimensional nucleation according to Avrami
A3 f = 3e·[-ln(e)]2/3  Three-dimensional nucleation according to Avrami
An f = n·e·[-ln(e)](n-1)/n  n-dimensional nucleation according to Avrami-Erofeev
Nk   Nakamura crystallization (Avrami + Hoffman-Lauritzen)
SbC   Sbirrazzuoli crystallization (Sestak-Berggren + Hoffman-Lauritzen)

*Kamal-Sourour (see references [1, 2]):

In case of projects of type DSC Curing, each reaction step can be described incorporating Diffusion Control.

 

Related Literature:

[1] S. Sourour, M.R. Kamal, Differential Scanning Calorimetry of Epoxy Cure: Isothermal Cure Kinetics, Thermochimica Acta 14 (1976), 41-59 

[2] B. Bilyeu, W. Brostow, K.P. Menard, Epoxy Thermosets and their applications III. Kinetic equations and models, Journal of Materials Education 23 (2001), 189-204