Files
opm-common/opm/material/eos/PengRobinsonMixture.hpp
Andreas Lauser 0f6540bdad DenseAD: make less fuzz about it
this patch converts to code to use the convenience functions instead
of the math toolboxes whereever possible. the main advantage is that
Opm::foo(x) will work regardless of the type of `x`, but it also
reduces visual clutter.

also, constant Evaluations are now directly created by assigning
Scalars, which removes further visual noise.

while I hope it improves the readability of the code,
functionality-wise this patch should not change anything.
2017-06-13 17:25:03 +02:00

166 lines
5.7 KiB
C++

// -*- 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::PengRobinsonMixture
*/
#ifndef OPM_PENG_ROBINSON_MIXTURE_HPP
#define OPM_PENG_ROBINSON_MIXTURE_HPP
#include "PengRobinson.hpp"
#include <opm/material/Constants.hpp>
#include <iostream>
namespace Opm {
/*!
* \brief Implements the Peng-Robinson equation of state for a
* mixture.
*/
template <class Scalar, class StaticParameters>
class PengRobinsonMixture
{
enum { numComponents = StaticParameters::numComponents };
typedef Opm::PengRobinson<Scalar> PengRobinson;
// this class cannot be instantiated!
PengRobinsonMixture() {}
// the ideal gas constant
static const Scalar R;
// the u and w parameters as given by the Peng-Robinson EOS
static const Scalar u;
static const Scalar w;
public:
/*!
* \brief Computes molar volumes where the Peng-Robinson EOS is
* true.
*
* \return Number of solutions.
*/
template <class MutableParams, class FluidState>
static int computeMolarVolumes(Scalar* Vm,
const MutableParams& params,
unsigned phaseIdx,
const FluidState& fs)
{
return PengRobinson::computeMolarVolumes(Vm, params, phaseIdx, fs);
}
/*!
* \brief Returns the fugacity coefficient of an individual
* component in the phase.
*
* The fugacity coefficient \f$\phi_i\f$ of a component \f$i\f$ is
* defined as
* \f[
f_i = \phi_i x_i \;,
\f]
* where \f$f_i\f$ is the component's fugacity and \f$x_i\f$ is
* the component's mole fraction.
*
* See:
*
* R. Reid, et al.: The Properties of Gases and Liquids,
* 4th edition, McGraw-Hill, 1987, pp. 42-44, 143-145
*/
template <class FluidState, class Params, class LhsEval = typename FluidState::Scalar>
static LhsEval computeFugacityCoefficient(const FluidState& fs,
const Params& params,
unsigned phaseIdx,
unsigned compIdx)
{
// note that we normalize the component mole fractions, so
// that their sum is 100%. This increases numerical stability
// considerably if the fluid state is not physical.
LhsEval Vm = params.molarVolume(phaseIdx);
// Calculate b_i / b
LhsEval bi_b = params.bPure(phaseIdx, compIdx) / params.b(phaseIdx);
// Calculate the compressibility factor
LhsEval RT = R*fs.temperature(phaseIdx);
LhsEval p = fs.pressure(phaseIdx); // molar volume in [bar]
LhsEval Z = p*Vm/RT; // compressibility factor
// Calculate A^* and B^* (see: Reid, p. 42)
LhsEval Astar = params.a(phaseIdx)*p/(RT*RT);
LhsEval Bstar = params.b(phaseIdx)*p/(RT);
// calculate delta_i (see: Reid, p. 145)
LhsEval sumMoleFractions = 0.0;
for (unsigned compJIdx = 0; compJIdx < numComponents; ++compJIdx)
sumMoleFractions += fs.moleFraction(phaseIdx, compJIdx);
LhsEval deltai = 2*Opm::sqrt(params.aPure(phaseIdx, compIdx))/params.a(phaseIdx);
LhsEval tmp = 0;
for (unsigned compJIdx = 0; compJIdx < numComponents; ++compJIdx) {
tmp +=
fs.moleFraction(phaseIdx, compJIdx)
/ sumMoleFractions
* Opm::sqrt(params.aPure(phaseIdx, compJIdx))
* (1.0 - StaticParameters::interactionCoefficient(compIdx, compJIdx));
};
deltai *= tmp;
LhsEval base =
(2*Z + Bstar*(u + std::sqrt(u*u - 4*w))) /
(2*Z + Bstar*(u - std::sqrt(u*u - 4*w)));
LhsEval expo = Astar/(Bstar*std::sqrt(u*u - 4*w))*(bi_b - deltai);
LhsEval fugCoeff =
Opm::exp(bi_b*(Z - 1))/Opm::max(1e-9, Z - Bstar) *
Opm::pow(base, expo);
////////
// limit the fugacity coefficient to a reasonable range:
//
// on one side, we want the mole fraction to be at
// least 10^-3 if the fugacity is at the current pressure
//
fugCoeff = Opm::min(1e10, fugCoeff);
//
// on the other hand, if the mole fraction of the component is 100%, we want the
// fugacity to be at least 10^-3 Pa
//
fugCoeff = Opm::max(1e-10, fugCoeff);
///////////
return fugCoeff;
}
};
template <class Scalar, class StaticParameters>
const Scalar PengRobinsonMixture<Scalar, StaticParameters>::R = Opm::Constants<Scalar>::R;
template<class Scalar, class StaticParameters>
const Scalar PengRobinsonMixture<Scalar, StaticParameters>::u = 2.0;
template<class Scalar, class StaticParameters>
const Scalar PengRobinsonMixture<Scalar, StaticParameters>::w = -1.0;
} // namespace Opm
#endif