RateES

Chemical Reactor Design Toolbox Reference Manual

ChemReactorDesign.Basic.Liquid.Rates.RateES

RateE.svg

Description

The component determines the molar fluxes due to a heterogeneous electrochemical reaction involving species in the solid and liquid phase

\begin{equation*}
\sum_{i}^{N^{S}} \nu_{i}^{S} \, A^{S}_{i}  + \sum_{i}^{N^{L}}} \nu^{L}_{k} \, A^{L}_{k}
+ n \, e^{-} = 0 
\end{equation*}

using a power law rate expression

\begin{equation*}
r = k(T) \, \left(
\exp\left\{-\alpha \, n \, f \, \eta(T) \right\} \, \for{\lambda}^{S} \, 
\prod_{i}^{N^{L}} a_{i}^{\for{\kappa_{i}}^{L}} \,
-
\exp\left\{(1-\alpha) \, n \, f \, \eta(T) \right\} \, \back{\lambda}^{S} \,
\prod_{i}^{N^{L}} a_{i}^{\back{\kappa_{i}}^{L}} \,
\right)
\end{equation*}

with

\begin{equation*}
a_{i}^{L} = \frac{\gamma_{i} \, c_{i}}{1 \, \frac{mol}{l}}
\end{equation*}

and

\begin{equation*}
f = \frac{\cal F}{R \, T}
\end{equation*}
\begin{equation*}
n = \lvert \sum_{i}^{N} \nu_{i} \, z_{i} \lvert
\end{equation*}

since for any solid species it holds

\begin{equation*}
a_{i}^{S} = 1 \quad \text{and} \quad \kappa_{i}^{S} = 0
\end{equation*}

The reference frame is set to the area of the electrode. The concentrations are obtained from the mole fractions and the temperature dependent molar volumes (c.f. getConc).

Temperature Dependent Parameters

  • Rate Constant

    \begin{equation*}
k(T) = k_{\infty} \, \exp\left\{-\frac{E_{a}}{R \, T} \right\}
\end{equation*}
  • Open Loop Potential

    \begin{equation*}
U_{0}(T) = - \frac{\sum\limits_{i}^{N} \nu_{i} \, \Delta G_{f_{i}}(T)}{n \, {\cal F}}
\end{equation*}
  • Overpotential

    \begin{equation*}
\eta(T) = U-U_{0}(T)
\end{equation*}

Comments

  • Generally, the reaction is regarded to be reversible. Thus, the individual orders of reaction are calculated from the provided stoichiometric coefficients to ensure equivalence between thermodynamics and kinetics.
  • As already mentioned, the reaction is of 0th order for any solid species involved. Thus, the rate should become zero if the amount of the respective solid species approaches zero. Therefore, respective boolean indicators are defined

    \begin{equation*}
{\for \lambda}^{S} = \left\{
\begin{array}{lcl}
0 & \text{if} & \sum\limits_{i}^{N}
\left(x_{i}^{S} \leq 0 \; \& \; \nu_{i}^{S} < 0 \right) > 0 \\
1 & \text{else} &
\end{array} \right.
\end{equation*}
    \begin{equation*}
{\back \lambda}^{S} = \left\{
\begin{array}{lcl}
0 & \text{if} & \sum\limits_{i}^{N}
\left(x_{i}^{S} \leq 0 \; \& \; \nu_{i}^{S} > 0 \right) > 0 \\
1 & \text{else} &
\end{array} \right.
\end{equation*}

    and incorporated in the rate expression for the forward and the backward reaction.

Variables

The molar fluxes for the liquid phase are obtained a

\begin{equation*}
F^{L}_{i} = \nu_{i} \,  A \, r
\qquad \text{for} \quad i=1,\cdots,N
\end{equation*}

and for the solid phase

\begin{equation*}
F^{S}_{i} = \nu^{S}_{i} \,  A \, r
\qquad \text{for} \quad i=1,\cdots,N^{S}
\end{equation*}

Since the heat of reaction, i.e. the energy change resulting from the change in composition, is implicitly accounted for in the balance equation of the respective volume component, it holds

\begin{equation*}
\Phi^{L} = 0 \qquad \text{and} \qquad \Phi^{S} = 0
\end{equation*}

The associated currrent is obtained as

\begin{equation*}
I = - {\cal F} \, \sum_{i}^{N} z_{i} \, F_{i}
\end{equation*}

Ports

Conserving

  • Liquid conserving port

    Port_B_L = Liquid;  %
    
  • Solid conserving port

    Port_B_S = Solid;  %
    
  • Electrical conserving ports

    Port_p = Electrical;  %
    
    Port_n = Electrical;  %
    

Input

  • Physical signal that represents the area

    A = {0,'m^2'}; % A
    

Parameters

Options

  • Option to select calculation of the open loop potential

    calculate_U0 = OnOff.Off;   
    

    On | Off

Kinetics

  • Frequency Factor

    kfinfA = {0,'mol/(cm^2*s)'};
    
  • Activation Energy

    Ea = {0,'kJ/mol'}; 
    
  • Factor of Symmetry

    alpha = {0.5,'1'};
    

Thermodynamics

  • Open Loop Potential

    U0 = {0,'V'};
    

    The parameter is only visible when the option calculate_U0 is set to On.

Liquid

  • Stoichiometric Coefficients

    nu = {[-1; 0],'1'};   
    

    Note Initially only two species are considered. As the number of species can be changed via the properties dialogue, the size of the array must be adjusted accordingly.

Solid

  • Stoichiometric Coefficients for Solid Phase

    nu_S = {[1;0],'1'}; 
    

    Notes Initially for the solid phase only two species are considered. As the number of species can be changed via the properties dialogue, the size of the array must be adjusted accordingly.

Nomenclature

\(A\) area
\(a_{i}\) activity of species Ai
\(c_i\) concentration of species Ai
\(E_{a}\) activation energy
\(F^{L}_{i}\) molar flow rate of species Ai in liquid phase
\(F^{S}_{i}\) molar flow rate of species Ai in solid phase
\(\Delta G_{f_{i}}\) Gibbs free energy of species Ai
\(I\) current
\(k\) reaction rate constant
\(n\) number of transferred electrons
\(N\) total number of species
\(r\) reaction rate
\(R\) universal gas constant
\(T\) temperature
\(U\) potential
\(U_{0}\) potential
\(x_{i}\) mole fraction of species Ai
\(z_{i}\) charge of species Ai
\(\cal F\) Faraday constant
\(\alpha\) symmetry factor
\(\eta\) overpotential
\(\nu_{i}\) stoichiometric coefficient of species Ai
\(\nu^{S}_{i}\) stoichiometric coefficient of species Ai in solid phase
\(\for{\kappa}_{i}\) order of reaction of species Ai (forward reaction)
\(\back{\kappa}_{i}\) order of reaction of species Ai (backward reaction)
\(\gamma_{i}\) activity coefficient of species Ai
\(\Phi^{L}\) energy flow rate in liquid phase
\(\Phi^{S}\) energy flow rate in solid phase