IonFlow.h

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//! @file IonFlow.h
 
// This file is part of Cantera. See License.txt in the top-level directory or
// at https://cantera.org/license.txt for license and copyright information.
 
#ifndef CT_IONFLOW_H
#define CT_IONFLOW_H
 
#include "cantera/oneD/Flow1D.h"
 
namespace Cantera
{
/**
 * This class models the ion transportation in a flame. There are three
 * stages of the simulation.
 *
 * The first stage turns off the diffusion of ions due to the fast
 * diffusion rate of electron without internal electric forces (ambi-
 * polar diffusion effect).
 *
 * The second stage evaluates drift flux from electric field calculated from
 * Poisson's equation, which is solved together with other equations. Poisson's
 * equation is coupled because the total charge densities depends on the species'
 * concentration. See Pedersen and Brown @cite pedersen1993 for details.
 *
 * @ingroup flowGroup
 */
class IonFlow : public Flow1D
{
public:
    IonFlow(ThermoPhase* ph = 0, size_t nsp = 1, size_t points = 1);
 
    //! Create a new flow domain.
    //! @param sol  Solution object used to evaluate all thermodynamic, kinetic, and
    //!     transport properties
    //! @param id  name of flow domain
    //! @param points  initial number of grid points
    IonFlow(shared_ptr<Solution> sol, const string& id="", size_t points = 1);
 
    string domainType() const override;
 
    size_t getSolvingStage() const override {
        return m_stage;
    }
    void setSolvingStage(const size_t stage) override;
 
    void resize(size_t components, size_t points) override;
    bool componentActive(size_t n) const override;
 
    void _finalize(const double* x) override;
 
    void solveElectricField(size_t j=npos) override;
    void fixElectricField(size_t j=npos) override;
    bool doElectricField(size_t j) const override {
        return m_do_electric_field[j];
    }
 
    /**
     * Sometimes it is desired to carry out the simulation using a specified
     * electron transport profile, rather than assuming it as a constant (0.4).
     * See Bisetti and El Morsli @cite bisetti2012.
     * If in the future the class GasTransport is improved, this method may
     * be discarded. This method specifies this profile.
    */
    void setElectronTransport(vector<double>& tfix,
                              vector<double>& diff_e,
                              vector<double>& mobi_e);
 
protected:
 
    /**
     * Evaluate the electric field equation residual by Gauss's law.
     *
     * The function calculates the electric field equation as:
     * @f[
     *    \frac{dE}{dz} = \frac{e}{\varepsilon_0} \sum (q_k \cdot n_k)
     * @f]
     *
     * and
     *
     * @f[
     *    E = -\frac{dV}{dz}
     * @f]
     *
     * The electric field equation is based on Gauss's law,
     * accounting for charge density and permittivity of free space
     * (@f$ \varepsilon_0 @f$).
     * The zero electric field is first evaluated and if the solution state is 2,
     * then the alternative form the electric field equation is evaluated.
     *
     * For argument explanation, see evalContinuity() base class.
     */
    void evalElectricField(double* x, double* rsd, int* diag,
                           double rdt, size_t jmin, size_t jmax) override;
 
    /**
     * Evaluate the species equations' residual. This function overloads the
     * original species function.
     *
     * A Neumann boundary for the charged species at the
     * left boundary is added, and the default boundary condition from the overloaded
     * method is left the same for the right boundary.
     *
     * For argument explanation, see evalContinuity() base class.
     */
    void evalSpecies(double* x, double* rsd, int* diag,
                     double rdt, size_t jmin, size_t jmax) override;
    void updateTransport(double* x, size_t j0, size_t j1) override;
    void updateDiffFluxes(const double* x, size_t j0, size_t j1) override;
    //! Solving phase one: the fluxes of charged species are turned off
    void frozenIonMethod(const double* x, size_t j0, size_t j1);
    //! Solving phase two: the electric field equation is added coupled
    //! by the electrical drift
    void electricFieldMethod(const double* x, size_t j0, size_t j1);
    //! flag for solving electric field or not
    vector<bool> m_do_electric_field;
 
    //! flag for importing transport of electron
    bool m_import_electron_transport = false;
 
    //! electrical properties
    vector<double> m_speciesCharge;
 
    //! index of species with charges
    vector<size_t> m_kCharge;
 
    //! index of neutral species
    vector<size_t> m_kNeutral;
 
    //! coefficients of polynomial fitting of fixed electron transport profile
    vector<double> m_mobi_e_fix;
    vector<double> m_diff_e_fix;
 
    //! mobility
    vector<double> m_mobility;
 
    //! solving stage
    size_t m_stage = 1;
 
    //! index of electron
    size_t m_kElectron = npos;
 
    //! electric field
    double E(const double* x, size_t j) const {
        return x[index(c_offset_E, j)];
    }
 
    double dEdz(const double* x, size_t j) const {
        return (E(x,j)-E(x,j-1))/(z(j)-z(j-1));
    }
 
    //! number density
    double ND(const double* x, size_t k, size_t j) const {
        return Avogadro * m_rho[j] * Y(x,k,j) / m_wt[k];
    }
 
    //! total charge density
    double rho_e(double* x, size_t j) const {
        double chargeDensity = 0.0;
        for (size_t k : m_kCharge) {
            chargeDensity += m_speciesCharge[k] * ElectronCharge * ND(x,k,j);
        }
        return chargeDensity;
    }
};
 
}
 
#endif