SLE

Chemical Reactor Design Toolbox Reference Manual

ChemReactorDesign.Basic.Liquid.Transfer.SLE

Partition.svg

Description

The component determines the molar flow rates of all species in the respective phases (solid and liquid) due to \(M\) individual solid-liquid equilibria (SLE).

The \(j^{th}\) dissolution is modelled as reversible reaction be

\begin{equation*}
A_{i}^{L} \rightleftharpoons A_{k}^{S}
\qquad \text{for} \qquad
j = 1,\cdots,M
\end{equation*}

Since for every equilibrium under consideration only one species per domain is involved, only one respective stoichiometric coefficient in the \(j^{th}\) mass transfer rate is different from zero. Using this criterion the relevant data are extracted and used in calculating the sorption rate.

The mass transfer rate is given as

\begin{equation*}
r_{j} = k_{j} \, \left( \lambda_{j}^{S} -
\frac{\gamma_{j}^{L} \, c_{i}^{L}}{K} \right)
\end{equation*}

with

\begin{equation*}
\lambda^{S}_{j} = \left\{
\begin{array}{ccc}
1 & \text{if} & c_{j}^{S} \geq 0 \\
0 & \text{else} &
\end{array}
\right.
\end{equation*}

Variables

The molar rates for both domains are given as

\begin{equation*}
F_{i}^{S} = A \, \sum_{j}^{M} \nu_{ij}^{S} \, r_{j}
\end{equation*}
\begin{equation*}
F_{i}^{L} = A \, \sum_{j}^{M} \nu_{ij}^{L} \, r_{j}
\end{equation*}

Since the heat transport associated with the mass transport is implicitly accounted for in the model equations of the associated balance component the energy flow rates become

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

Ports

Conserving

  • Liquid 1 conserving port

    Port_B1 = Liquid;  %
    
  • Liquid 2 conserving port

    Port_B1 = Gas;  %
    

Input

  • Physical signal that represents the surface area

    Ain = {0,'m^2'};
    

    Dependencies: The port is only visible when areaInput is set to On.

Parameters

Options

  • Option to select area input

    areaInput = OnOff.Off;
    

    Off | On

Geometry

  • Surface Area

    A0 = {0,'cm^2'}; 
    

    Dependencies: The parameter is only visible when the option areaInput is set to Off.

Stoichiometry

  • Stoichiometric coefficients for solid domain

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

    Note Initially only one equilibrium is considered. When the number of individual equilibria is increased, the size of the array must be adjusted accordingly.

  • Stoichiometric coefficients for liquid domain

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

    Note Initially only one equilibrium is considered. When the number of individual equilibria is increased, the size of the array must be adjusted accordingly.

Thermodynamics

  • Equilibrium constant

    K0 = {1,'1'};  
    

    Note Initially, only one equilibrium is considered. When the number is increased, the size of the array must be adjusted accordingly.

Kinetics

  • Rate constants

    k = {0,'mol/(m^2*s)'}; 
    

    Note Initially only one equilibrium is considered. When the number of individual equilibria is increased, the size of the array must be adjusted accordingly.

Nomenclature

\(A\) area
\(F_{i}\) molar flow rate of species Ai
\({\Delta_{f} H}\) molar enthalpy of species Ai
\(K\) equilibrium constant
\(k\) rate constant
\(N\) total number of species
\(M\) number of equlibria
\(p\) pressure
\(r\) mass transfer rate
\(R\) universal gas constant
\(T\) temperature
\(x_{i}\) mole fraction of species Ai
\(\Phi\) energy flow rate
\(\gamma\) activity coefficient of species Ai