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opm-common/opm/material/components/N2.hpp
2022-08-02 10:16:25 +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::N2
*/
#ifndef OPM_N2_HPP
#define OPM_N2_HPP
#include "Component.hpp"
#include <opm/material/IdealGas.hpp>
#include <opm/material/common/MathToolbox.hpp>
#include <cmath>
namespace Opm
{
/*!
* \ingroup Components
*
* \brief Properties of pure molecular nitrogen \f$N_2\f$.
*
* \tparam Scalar The type used for scalar values
*/
template <class Scalar>
class N2 : public Component<Scalar, N2<Scalar> >
{
typedef ::Opm::IdealGas<Scalar> IdealGas;
public:
/*!
* \brief A human readable name for nitrogen.
*/
static const char* name()
{ return "N2"; }
/*!
* \brief The molar mass in \f$\mathrm{[kg/mol]}\f$ of molecular nitrogen.
*/
static Scalar molarMass()
{ return 28.0134e-3;}
/*!
* \brief Returns the critical temperature \f$\mathrm{[K]}\f$ of molecular nitrogen
*/
static Scalar criticalTemperature()
{ return 126.192; /* [K] */ }
/*!
* \brief Returns the critical pressure \f$\mathrm{[Pa]}\f$ of molecular nitrogen.
*/
static Scalar criticalPressure()
{ return 3.39858e6; /* [N/m^2] */ }
/*!
* \brief Critical volume of \f$N_2\f$ [m2/kmol].
*/
static Scalar criticalVolume() {return 8.94e-2; }
/*!
* \brief Acentric factor of \f$N_2\f$.
*/
static Scalar acentricFactor() { return 0.039; }
/*!
* \brief Returns the temperature \f$\mathrm{[K]}\f$ at molecular nitrogen's triple point.
*/
static Scalar tripleTemperature()
{ return 63.151; /* [K] */ }
/*!
* \brief Returns the pressure \f$\mathrm{[Pa]}\f$ at molecular nitrogen's triple point.
*/
static Scalar triplePressure()
{ return 12.523e3; /* [N/m^2] */ }
/*!
* \brief The vapor pressure in \f$\mathrm{[Pa]}\f$ of pure molecular nitrogen
* at a given temperature.
*
*\param temperature temperature of component in \f$\mathrm{[K]}\f$
*
* Taken from:
*
* R. Span, E.W. Lemmon, et al.: "A Reference Equation of State
* for the Thermodynamic Properties of Nitrogen for Temperatures
* from 63.151 to 1000 K and Pressures to 2200 MPa", Journal of
* Physical and Chemical Refefence Data, Vol. 29, No. 6,
* pp. 1361-1433
*/
template <class Evaluation>
static Evaluation vaporPressure(const Evaluation& temperature)
{
if (temperature > criticalTemperature())
return criticalPressure();
if (temperature < tripleTemperature())
return 0; // N2 is solid: We don't take sublimation into
// account
// note: this is the ancillary equation given on page 1368
const Evaluation& sigma = 1.0 - temperature/criticalTemperature();
const Evaluation& sqrtSigma = sqrt(sigma);
const Scalar N1 = -6.12445284;
const Scalar N2 = 1.26327220;
const Scalar N3 = -0.765910082;
const Scalar N4 = -1.77570564;
return
criticalPressure() *
exp(criticalTemperature()/temperature*
(sigma*(N1 +
sqrtSigma*N2 +
sigma*(sqrtSigma*N3 +
sigma*sigma*sigma*N4))));
}
/*!
* \brief The density \f$\mathrm{[kg/m^3]}\f$ of \f$N_2\f$ gas 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(const Evaluation& temperature, const Evaluation& pressure)
{
// Assume an ideal gas
return IdealGas::density(Evaluation(molarMass()), temperature, pressure);
}
/*!
* \brief Returns true iff the gas phase is assumed to be compressible
*/
static bool gasIsCompressible()
{ return true; }
/*!
* \brief Returns true iff the gas phase is assumed to be ideal
*/
static bool gasIsIdeal()
{ return true; }
/*!
* \brief The pressure of gaseous \f$N_2\f$ 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(const Evaluation& temperature, const Evaluation& density)
{
// Assume an ideal gas
return IdealGas::pressure(temperature, density/molarMass());
}
/*!
* \brief Specific enthalpy \f$\mathrm{[J/kg]}\f$ of pure nitrogen gas.
*
* \param temperature temperature of component in \f$\mathrm{[K]}\f$
* \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
*
* See: R. Reid, et al.: The Properties of Gases and Liquids, 4th
* edition, McGraw-Hill, 1987, pp 154, 657, 665
*/
template <class Evaluation>
static Evaluation gasEnthalpy(const Evaluation& temperature,
const Evaluation&)
{
// method of Joback
const Scalar cpVapA = 31.15;
const Scalar cpVapB = -0.01357;
const Scalar cpVapC = 2.680e-5;
const Scalar cpVapD = -1.168e-8;
// calculate: \int_0^T c_p dT
return
1/molarMass()* // conversion from [J/(mol K)] to [J/(kg K)]
temperature*(cpVapA + temperature*
(cpVapB/2 + temperature*
(cpVapC/3 + temperature*
(cpVapD/4))));
}
/*!
* \brief Specific enthalpy \f$\mathrm{[J/kg]}\f$ of pure nitrogen gas.
*
* Definition of enthalpy: \f$h= u + pv = u + p / \rho\f$.
*
* Rearranging for internal energy yields: \f$u = h - pv\f$.
*
* Exploiting the Ideal Gas assumption (\f$pv = R_{\textnormal{specific}} T\f$)gives: \f$u = h - R / M T \f$.
*
* The universal gas constant can only be used in the case of molar formulations.
* \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 gasInternalEnergy(const Evaluation& temperature,
const Evaluation& pressure)
{
return
gasEnthalpy(temperature, pressure) -
1/molarMass()* // conversion from [J/(mol K)] to [J/(kg K)]
IdealGas::R*temperature; // = pressure * spec. volume for an ideal gas
}
/*!
* \brief Specific isobaric heat capacity \f$[J/(kg K)]\f$ of pure
* nitrogen gas.
*
* This is equivalent to the partial derivative of the specific
* enthalpy to the temperature.
*/
template <class Evaluation>
static Evaluation gasHeatCapacity(const Evaluation& temperature,
const Evaluation&)
{
// method of Joback
const Scalar cpVapA = 31.15;
const Scalar cpVapB = -0.01357;
const Scalar cpVapC = 2.680e-5;
const Scalar cpVapD = -1.168e-8;
return
1/molarMass()* // conversion from [J/(mol K)] to [J/(kg K)]
cpVapA + temperature*
(cpVapB + temperature*
(cpVapC + temperature*
(cpVapD)));
}
/*!
* \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of \f$N_2\f$ 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 = 90.1; // critical specific volume [cm^3/mol]
const Scalar omega = 0.037; // 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 heat conductivity of steam \f$\mathrm{[W/(m K)]}\f$.
*
* Isobaric Properties for Nitrogen in: NIST Standard Reference
* Database Number 69, Eds. P.J. Linstrom and W.G. Mallard
* evaluated at p=.1 MPa, T=8°C, does not change dramatically with
* p,T
*
* \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 gasThermalConductivity(const Evaluation& /*temperature*/,
const Evaluation& /*pressure*/)
{ return 0.024572; }
};
} // namespace Opm
#endif