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- make the methods of the fluid systems and components which just return a parameter constexpr. - don't use 'const' for call-by value parameters
88 lines
3.3 KiB
C++
88 lines
3.3 KiB
C++
// -*- mode: C++; tab-width: 4; indent-tabs-mode: nil; c-basic-offset: 4 -*-
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// vi: set et ts=4 sw=4 sts=4:
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/*****************************************************************************
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* Copyright (C) 2009 by Andreas Lauser *
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* Institute for Modelling Hydraulic and Environmental Systems *
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* University of Stuttgart, Germany *
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* email: <givenname>.<name>@iws.uni-stuttgart.de *
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* *
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* This program is free software: you can redistribute it and/or modify *
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* it under the terms of the GNU General Public License as published by *
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* the Free Software Foundation, either version 2 of the License, or *
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* (at your option) any later version. *
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* *
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* This program is distributed in the hope that it will be useful, *
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* but WITHOUT ANY WARRANTY; without even the implied warranty of *
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* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the *
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* GNU General Public License for more details. *
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* *
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* You should have received a copy of the GNU General Public License *
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* along with this program. If not, see <http://www.gnu.org/licenses/>. *
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*****************************************************************************/
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/*!
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* \file
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*
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* \brief The IAPWS formulation of Henry coefficients in water.
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*/
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#ifndef DUMUX_HENRY_IAPWS_HH
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#define DUMUX_HENRY_IAPWS_HH
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#include <dumux/material/components/h2o.hh>
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namespace Dumux
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{
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/*!
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* \ingroup Binarycoefficients
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* \brief The Henry constants in liquid water using the IAPWS 2004
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* formulation.
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*
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* This function calculates \f$K_D\f$, see:
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*
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* IAPWS: "Guideline on the Henry's Constant and Vapor-Liquid
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* Distribution Constant for Gases in H2O and D2O at High
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* Temperatures"
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* http://www.iapws.org/relguide/HenGuide.pdf
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*/
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template <class Scalar>
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inline Scalar henryIAPWS(Scalar E,
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Scalar F,
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Scalar G,
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Scalar H,
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Scalar temperature)
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{
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typedef Dumux::H2O<Scalar> H2O;
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Scalar Tr = temperature/H2O::criticalTemperature();
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Scalar tau = 1 - Tr;
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static constexpr Scalar c[6] = {
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1.99274064, 1.09965342, -0.510839303,
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-1.75493479,-45.5170352, -6.7469445e5
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};
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static constexpr Scalar d[6] = {
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1/3.0, 2/3.0, 5/3.0,
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16/3.0, 43/3.0, 110/3.0
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};
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static constexpr Scalar q = -0.023767;
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Scalar f = 0;
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for (int i = 0; i < 6; ++i) {
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f += c[i]*std::pow(tau, d[i]);
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}
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Scalar exponent =
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q*F +
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E/temperature*f +
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(F +
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G*std::pow(tau, 2.0/3) +
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H*tau)*
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std::exp((H2O::tripleTemperature() - temperature)/100);
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// CAUTION: K_D is formulated in mole fractions. We have to
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// multiply it with the vapor pressure of water in order to get
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// derivative of the partial pressure.
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return std::exp(exponent)*H2O::vaporPressure(temperature);
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}
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}
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#endif // DUMUX_HENRY_IAPWS_HH
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