conceptually, this may not be the purest conceivable solution, but it is the most practical one.
119 lines
4.0 KiB
C++
119 lines
4.0 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) 2009-2013 by Andreas Lauser
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Copyright (C) 2010 by Felix Bode
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Copyright (C) 2010 by Benjamin Faigle
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This file is part of the Open Porous Media project (OPM).
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OPM 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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OPM 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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You should have received a copy of the GNU General Public License
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along with OPM. 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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* \copydoc Opm::BinaryCoeff::H2O_Air
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*/
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#ifndef OPM_BINARY_COEFF_H2O_AIR_HPP
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#define OPM_BINARY_COEFF_H2O_AIR_HPP
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#include <opm/material/common/MathToolbox.hpp>
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#include <cmath>
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namespace Opm {
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namespace BinaryCoeff {
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/*!
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* \ingroup Binarycoefficients
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* \brief Binary coefficients for water and nitrogen.
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*/
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class H2O_Air
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{
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public:
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/*!
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* \brief Henry coefficent \f$\mathrm{[N/m^2]}\f$ for air in liquid water.
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*
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*
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* Henry coefficent See:
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* Stefan Finsterle, 1993
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* Inverse Modellierung zur Bestimmung hydrogeologischer Parameter eines Zweiphasensystems
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* page 29 Formula (2.9) (nach Tchobanoglous & Schroeder, 1985)
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*
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*/
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template <class Evaluation>
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static Evaluation henry(const Evaluation& temperature)
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{
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typedef Opm::MathToolbox<Evaluation> Toolbox;
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return 1.0/((0.8942+1.47*Toolbox::exp(-0.04394*(temperature-273.15)))*1.E-10);
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}
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/*!
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* \brief Binary diffusion coefficent \f$\mathrm{[m^2/s]}\f$ for molecular water and air
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*
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* \param temperature the temperature \f$\mathrm{[K]}\f$
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* \param pressure the phase pressure \f$\mathrm{[Pa]}\f$
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* Vargaftik : Tables on the thermophysical properties of liquids and gases. John Wiley & * Sons, New York, 1975.
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*
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* Walker, Sabey, Hampton: Studies of heat transfer and water migration in soils.
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* Dep. of Agricultural and Chemical Engineering, Colorado State University,
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* Fort Collins, 1981.
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*/
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template <class Evaluation>
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static Evaluation gasDiffCoeff(const Evaluation& temperature, const Evaluation& pressure)
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{
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typedef Opm::MathToolbox<Evaluation> Toolbox;
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double Theta=1.8;
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double Daw=2.13e-5; /* reference value */
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double pg0=1.e5; /* reference pressure */
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double T0=273.15; /* reference temperature */
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return Daw*(pg0/pressure)*Toolbox::pow((temperature/T0),Theta);
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}
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/*!
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* Lacking better data on water-air diffusion in liquids, we use at the
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* moment the diffusion coefficient of the air's main component nitrogen!!
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* \brief Diffusion coefficent \f$\mathrm{[m^2/s]}\f$ for molecular nitrogen in liquid water.
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*
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* The empirical equations for estimating the diffusion coefficient in
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* infinite solution which are presented in Reid, 1987 all show a
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* linear dependency on temperature. We thus simply scale the
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* experimentally obtained diffusion coefficient of Ferrell and
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* Himmelblau by the temperature.
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*
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* See:
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*
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* R. Reid et al.: "The properties of Gases and Liquids", 4th edition,
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* pp. 599, McGraw-Hill, 1987
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*
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* R. Ferrell, D. Himmelblau: "Diffusion Coeffients of Nitrogen and
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* Oxygen in Water", Journal of Chemical Engineering and Data,
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* Vol. 12, No. 1, pp. 111-115, 1967
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*/
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template <class Evaluation>
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static Evaluation liquidDiffCoeff(const Evaluation& temperature, const Evaluation& pressure)
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{
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const double Texp = 273.15 + 25; // [K]
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const double Dexp = 2.01e-9; // [m^2/s]
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return Dexp/Texp*temperature;
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}
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};
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} // namespace BinaryCoeff
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} // namespace Opm
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#endif
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