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opm-common/opm/material/components/H2.hpp
2023-04-12 14:28:01 +02:00

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// -*- mode: C++; tab-width: 4; indent-tabs-mode: nil; c-basic-offset: 4 -*-
// vi: set et ts=4 sw=4 sts=4:
/*
This file is part of the Open Porous Media project (OPM).
OPM is free software: you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation, either version 2 of the License, or
(at your option) any later version.
OPM is distributed in the hope that it will be useful,
but WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
GNU General Public License for more details.
You should have received a copy of the GNU General Public License
along with OPM. If not, see <http://www.gnu.org/licenses/>.
Consult the COPYING file in the top-level source directory of this
module for the precise wording of the license and the list of
copyright holders.
*/
/*!
* \file
* \copydoc Opm:H2
* \brief Properties of pure molecular hydrogen \f$H_2\f$.
*/
#ifndef OPM_H2_HPP
#define OPM_H2_HPP
#include <opm/material/IdealGas.hpp>
#include <opm/material/components/Component.hpp>
#include <opm/material/densead/Math.hpp>
#include <cmath>
namespace Opm {
/*!
* \ingroup Components
* \brief Properties of pure molecular hydrogen \f$H_2\f$.
*
* \tparam Scalar The type used for scalar values
*/
template <class Scalar>
class H2 : public Component<Scalar, H2<Scalar> >
{
using IdealGas = Opm::IdealGas<Scalar>;
public:
/*!
* \brief A human readable name for the \f$H_2\f$.
*/
static std::string name()
{ return "H2"; }
/*!
* \brief The molar mass in \f$\mathrm{[kg/mol]}\f$ of molecular hydrogen.
*/
static constexpr Scalar molarMass()
{ return 2.01588e-3; }
/*!
* \brief Returns the critical temperature \f$\mathrm{[K]}\f$ of molecular hydrogen.
*/
static Scalar criticalTemperature()
{ return 33.2; /* [K] */ }
/*!
* \brief Returns the critical pressure \f$\mathrm{[Pa]}\f$ of molecular hydrogen.
*/
static Scalar criticalPressure()
{ return 13.0e5; /* [N/m^2] */ }
/*!
* \brief Returns the critical density \f$\mathrm{[mol/cm^3]}\f$ of molecular hydrogen.
*/
static Scalar criticalDensity()
{ return 15.508e-3; /* [mol/cm^3] */ }
/*!
* \brief Returns the temperature \f$\mathrm{[K]}\f$ at molecular hydrogen's triple point.
*/
static Scalar tripleTemperature()
{ return 14.0; /* [K] */ }
/*!
* \brief The vapor pressure in \f$\mathrm{[Pa]}\f$ of pure molecular hydrogen
* at a given temperature.
*
*\param temperature temperature of component in \f$\mathrm{[K]}\f$
*
* Taken from:
*
* See: R. Reid, et al. (1987, pp 208-209, 669) \cite reid1987
*
* \todo implement the Gomez-Thodos approach...
*/
template <class Evaluation>
static Evaluation vaporPressure(Evaluation temperature)
{
if (temperature > criticalTemperature())
return criticalPressure();
if (temperature < tripleTemperature())
return 0; // H2 is solid: We don't take sublimation into
// account
// antoine equation
const Scalar A = -7.76451;
const Scalar B = 1.45838;
const Scalar C = -2.77580;
return 1e5 * exp(A - B/(temperature + C));
}
/*!
* \brief The density \f$\mathrm{[kg/m^3]}\f$ of \f$H_2\f$ at a given pressure and temperature.
*
* \param temperature temperature of component in \f$\mathrm{[K]}\f$
* \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
*/
template <class Evaluation>
static Evaluation gasDensity(Evaluation temperature, Evaluation pressure)
{
// Assume an ideal gas
return IdealGas::density(Evaluation(molarMass()), temperature, pressure);
}
/*!
* \brief The molar density of \f$H_2\f$ in \f$\mathrm{[mol/m^3]}\f$,
* depending on pressure and temperature.
* \param temperature The temperature of the gas
* \param pressure The pressure of the gas
*/
template <class Evaluation>
static Evaluation gasMolarDensity(Evaluation temperature, Evaluation pressure)
{ return IdealGas::molarDensity(temperature, pressure); }
/*!
* \brief Returns true if the gas phase is assumed to be compressible
*/
static constexpr bool gasIsCompressible()
{ return true; }
/*!
* \brief Returns true if the gas phase is assumed to be ideal
*/
static constexpr bool gasIsIdeal()
{ return true; }
/*!
* \brief The pressure of gaseous \f$H_2\f$ in \f$\mathrm{[Pa]}\f$ at a given density and temperature.
*
* \param temperature temperature of component in \f$\mathrm{[K]}\f$
* \param density density of component in \f$\mathrm{[kg/m^3]}\f$
*/
template <class Evaluation>
static Evaluation gasPressure(Evaluation temperature, Evaluation density)
{
// Assume an ideal gas
return IdealGas::pressure(temperature, density/molarMass());
}
/*!
* \brief Specific internal energy of H2 [J/kg].
*/
template <class Evaluation>
static Evaluation gasInternalEnergy(const Evaluation& temperature,
const Evaluation& pressure)
{
const Evaluation& h = gasEnthalpy(temperature, pressure);
const Evaluation& rho = gasDensity(temperature, pressure);
return h - (pressure / rho);
}
/*!
* \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of \f$H_2\f$ at a given pressure and temperature.
*
* \param temperature temperature of component in \f$\mathrm{[K]}\f$
* \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
*
* See:
*
* See: R. Reid, et al.: The Properties of Gases and Liquids,
* 4th edition, McGraw-Hill, 1987, pp 396-397,
* 5th edition, McGraw-Hill, 2001 pp 9.7-9.8 (omega and V_c taken from p. A.19)
*
*/
template <class Evaluation>
static Evaluation gasViscosity(const Evaluation& temperature, const Evaluation& /*pressure*/)
{
const Scalar Tc = criticalTemperature();
const Scalar Vc = 64.2; // critical specific volume [cm^3/mol]
const Scalar omega = -0.217; // accentric factor
const Scalar M = molarMass() * 1e3; // molar mas [g/mol]
const Scalar dipole = 0.0; // dipole moment [debye]
Scalar mu_r4 = 131.3 * dipole / std::sqrt(Vc * Tc);
mu_r4 *= mu_r4;
mu_r4 *= mu_r4;
Scalar Fc = 1 - 0.2756*omega + 0.059035*mu_r4;
const Evaluation& Tstar = 1.2593 * temperature/Tc;
const Evaluation& Omega_v =
1.16145*pow(Tstar, -0.14874) +
0.52487*exp(- 0.77320*Tstar) +
2.16178*exp(- 2.43787*Tstar);
const Evaluation& mu = 40.785*Fc*sqrt(M*temperature)/(std::pow(Vc, 2./3)*Omega_v);
// convertion from micro poise to Pa s
return mu/1e6 / 10;
}
/*!
* \brief Specific enthalpy \f$\mathrm{[J/kg]}\f$ of pure hydrogen gas.
*
* \param temperature temperature of component in \f$\mathrm{[K]}\f$
* \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
*/
template <class Evaluation>
static const Evaluation gasEnthalpy(Evaluation temperature,
Evaluation pressure)
{
return gasHeatCapacity(temperature, pressure) * temperature;
}
/*!
* \brief Specific isobaric heat capacity \f$\mathrm{[J/(kg*K)]}\f$ of pure
* hydrogen gas.
*
* This is equivalent to the partial derivative of the specific
* enthalpy to the temperature.
* \param T temperature of component in \f$\mathrm{[K]}\f$
* \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
*
* See: R. Reid, et al. (1987, pp 154, 657, 665) \cite reid1987
*/
template <class Evaluation>
static const Evaluation gasHeatCapacity(Evaluation T,
Evaluation pressure)
{
// method of Joback
const Scalar cpVapA = 27.14;
const Scalar cpVapB = 9.273e-3;
const Scalar cpVapC = -1.381e-5;
const Scalar cpVapD = 7.645e-9;
return
1/molarMass()* // conversion from [J/(mol*K)] to [J/(kg*K)]
(cpVapA + T*
(cpVapB/2 + T*
(cpVapC/3 + T*
(cpVapD/4))));
}
};
} // end namespace Opm
#endif