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1 | // -*- mode: C++; tab-width: 4; indent-tabs-mode: nil; c-basic-offset: 4 -*- | ||
2 | // vi: set et ts=4 sw=4 sts=4: | ||
3 | // | ||
4 | // SPDX-FileCopyrightInfo: Copyright © DuMux Project contributors, see AUTHORS.md in root folder | ||
5 | // SPDX-License-Identifier: GPL-3.0-or-later | ||
6 | // | ||
7 | /*! | ||
8 | * \file | ||
9 | * \ingroup Components | ||
10 | * \brief Properties of pure molecular nitrogen \f$N_2\f$. | ||
11 | */ | ||
12 | #ifndef DUMUX_N2_HH | ||
13 | #define DUMUX_N2_HH | ||
14 | |||
15 | #include <dumux/material/idealgas.hh> | ||
16 | |||
17 | #include <cmath> | ||
18 | |||
19 | #include <dumux/material/components/base.hh> | ||
20 | #include <dumux/material/components/gas.hh> | ||
21 | |||
22 | namespace Dumux { | ||
23 | namespace Components { | ||
24 | |||
25 | /*! | ||
26 | * \ingroup Components | ||
27 | * \brief Properties of pure molecular nitrogen \f$N_2\f$. | ||
28 | * | ||
29 | * \tparam Scalar The type used for scalar values | ||
30 | */ | ||
31 | template <class Scalar> | ||
32 | class N2 | ||
33 | : public Components::Base<Scalar, N2<Scalar> > | ||
34 | , public Components::Gas<Scalar, N2<Scalar> > | ||
35 | { | ||
36 | using IdealGas = Dumux::IdealGas<Scalar>; | ||
37 | |||
38 | public: | ||
39 | /*! | ||
40 | * \brief A human readable name for nitrogen. | ||
41 | */ | ||
42 | static std::string name() | ||
43 |
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|
404 | { return "N2"; } |
44 | |||
45 | /*! | ||
46 | * \brief The molar mass in \f$\mathrm{[kg/mol]}\f$ of molecular nitrogen. | ||
47 | */ | ||
48 | static constexpr Scalar molarMass() | ||
49 | { return 28.0134e-3;} | ||
50 | |||
51 | /*! | ||
52 | * \brief Returns the critical temperature \f$\mathrm{[K]}\f$ of molecular nitrogen | ||
53 | */ | ||
54 | static Scalar criticalTemperature() | ||
55 | { return 126.192; /* [K] */ } | ||
56 | |||
57 | /*! | ||
58 | * \brief Returns the critical pressure \f$\mathrm{[Pa]}\f$ of molecular nitrogen. | ||
59 | */ | ||
60 | static Scalar criticalPressure() | ||
61 | { return 3.39858e6; /* [N/m^2] */ } | ||
62 | |||
63 | /*! | ||
64 | * \brief Returns the temperature \f$\mathrm{[K]}\f$ at molecular nitrogen's triple point. | ||
65 | */ | ||
66 | static Scalar tripleTemperature() | ||
67 | { return 63.151; /* [K] */ } | ||
68 | |||
69 | /*! | ||
70 | * \brief Returns the pressure \f$\mathrm{[Pa]}\f$ at molecular nitrogen's triple point. | ||
71 | */ | ||
72 | static Scalar triplePressure() | ||
73 | { return 12.523e3; /* [N/m^2] */ } | ||
74 | |||
75 | /*! | ||
76 | * \brief The vapor pressure in \f$\mathrm{[Pa]}\f$ of pure molecular nitrogen | ||
77 | * at a given temperature. | ||
78 | * | ||
79 | * \param T temperature of component in \f$\mathrm{[K]}\f$ | ||
80 | * | ||
81 | * Taken from: | ||
82 | * | ||
83 | * R. Span, E.W. Lemmon, et al. (2000 ,pp. 1361-1433) \cite span2000 | ||
84 | */ | ||
85 | 3 | static Scalar vaporPressure(Scalar T) | |
86 | { | ||
87 |
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3 | if (T > criticalTemperature()) |
88 | return criticalPressure(); | ||
89 | ✗ | if (T < tripleTemperature()) | |
90 | return 0; // N2 is solid: We don't take sublimation into | ||
91 | // account | ||
92 | |||
93 | // note: this is the ancillary equation given on page 1368 | ||
94 | using std::sqrt; | ||
95 | ✗ | Scalar sigma = Scalar(1.0) - T/criticalTemperature(); | |
96 | ✗ | Scalar sqrtSigma = sqrt(sigma); | |
97 | ✗ | const Scalar N1 = -6.12445284; | |
98 | ✗ | const Scalar N2 = 1.26327220; | |
99 | ✗ | const Scalar N3 = -0.765910082; | |
100 | ✗ | const Scalar N4 = -1.77570564; | |
101 | |||
102 | using std::exp; | ||
103 | return | ||
104 | ✗ | criticalPressure() * | |
105 | ✗ | exp(criticalTemperature()/T* | |
106 | ✗ | (sigma*(N1 + | |
107 | ✗ | sqrtSigma*N2 + | |
108 | ✗ | sigma*(sqrtSigma*N3 + | |
109 | ✗ | sigma*sigma*sigma*N4)))); | |
110 | } | ||
111 | |||
112 | /*! | ||
113 | * \brief The density \f$\mathrm{[kg/m^3]}\f$ of \f$N_2\f$ gas at a given pressure and temperature. | ||
114 | * | ||
115 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
116 | * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$ | ||
117 | */ | ||
118 | static Scalar gasDensity(Scalar temperature, Scalar pressure) | ||
119 | { | ||
120 | // Assume an ideal gas | ||
121 |
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23697846 | return IdealGas::density(molarMass(), temperature, pressure); |
122 | } | ||
123 | |||
124 | /*! | ||
125 | * \brief The molar density of \f$N_2\f$ gas in \f$\mathrm{[mol/m^3]}\f$ at a given pressure and temperature. | ||
126 | * | ||
127 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
128 | * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$ | ||
129 | * | ||
130 | */ | ||
131 | static Scalar gasMolarDensity(Scalar temperature, Scalar pressure) | ||
132 | 23697620 | { return IdealGas::molarDensity(temperature, pressure); } | |
133 | |||
134 | /*! | ||
135 | * \brief Returns true if the gas phase is assumed to be compressible | ||
136 | */ | ||
137 | static constexpr bool gasIsCompressible() | ||
138 | { return true; } | ||
139 | |||
140 | /*! | ||
141 | * \brief Returns true if the gas phase is assumed to be ideal | ||
142 | */ | ||
143 | static constexpr bool gasIsIdeal() | ||
144 | { return true; } | ||
145 | |||
146 | /*! | ||
147 | * \brief The pressure of gaseous \f$N_2\f$ in \f$\mathrm{[Pa]}\f$ at a given density and temperature. | ||
148 | * | ||
149 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
150 | * \param density density of component in \f$\mathrm{[kg/m^3]}\f$ | ||
151 | */ | ||
152 | static Scalar gasPressure(Scalar temperature, Scalar density) | ||
153 | { | ||
154 | // Assume an ideal gas | ||
155 | 18 | return IdealGas::pressure(temperature, density/molarMass()); | |
156 | } | ||
157 | |||
158 | /*! | ||
159 | * \brief Specific enthalpy \f$\mathrm{[J/kg]}\f$ of pure nitrogen gas. | ||
160 | * | ||
161 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
162 | * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$ | ||
163 | */ | ||
164 | ✗ | static const Scalar gasEnthalpy(Scalar temperature, | |
165 | Scalar pressure) | ||
166 | { | ||
167 | 42257582 | return gasHeatCapacity(temperature, pressure) * temperature; | |
168 | } | ||
169 | |||
170 | /*! | ||
171 | * \brief Specific enthalpy \f$\mathrm{[J/kg]}\f$ of pure nitrogen gas. | ||
172 | * | ||
173 | * Definition of enthalpy: \f$h= u + pv = u + p / \rho\f$. | ||
174 | * | ||
175 | * Rearranging for internal energy yields: \f$u = h - pv\f$. | ||
176 | * | ||
177 | * Exploiting the Ideal Gas assumption (\f$pv = R_{\textnormal{specific}} T\f$)gives: \f$u = h - R / M T \f$. | ||
178 | * | ||
179 | * The universal gas constant can only be used in the case of molar formulations. | ||
180 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
181 | * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$ | ||
182 | */ | ||
183 | static const Scalar gasInternalEnergy(Scalar temperature, | ||
184 | Scalar pressure) | ||
185 | { | ||
186 | return | ||
187 | gasEnthalpy(temperature, pressure) - | ||
188 | 1/molarMass()* // conversion from [J/(mol K)] to [J/(kg K)] | ||
189 | IdealGas::R*temperature; // = pressure * spec. volume for an ideal gas | ||
190 | } | ||
191 | |||
192 | /*! | ||
193 | * \brief Specific isobaric heat capacity \f$\mathrm{[J/(kg*K)]}\f$ of pure | ||
194 | * nitrogen gas. | ||
195 | * | ||
196 | * This is equivalent to the partial derivative of the specific | ||
197 | * enthalpy to the temperature. | ||
198 | * | ||
199 | * See: R. Reid, et al. (1987, pp 154, 657, 665) \cite reid1987 | ||
200 | */ | ||
201 | ✗ | static const Scalar gasHeatCapacity(Scalar T, | |
202 | Scalar pressure) | ||
203 | { | ||
204 | // method of Joback | ||
205 | 21128909 | const Scalar cpVapA = 31.15; | |
206 | 21128909 | const Scalar cpVapB = -0.01357; | |
207 | 21128909 | const Scalar cpVapC = 2.680e-5; | |
208 | 21128909 | const Scalar cpVapD = -1.168e-8; | |
209 | |||
210 | return | ||
211 | 1/molarMass()* // conversion from [J/(mol K)] to [J/(kg K)] | ||
212 | 21128909 | (cpVapA + T* | |
213 | 21128909 | (cpVapB/2 + T* | |
214 | 21128909 | (cpVapC/3 + T* | |
215 | 21128909 | (cpVapD/4)))); | |
216 | } | ||
217 | |||
218 | /*! | ||
219 | * \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of \f$N_2\f$ at a given pressure and temperature. | ||
220 | * | ||
221 | * \param temperature temperature of component in \f$\mathrm{[K]}\f$ | ||
222 | * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$ | ||
223 | * | ||
224 | * See: | ||
225 | * | ||
226 | * See: R. Reid, et al.: The Properties of Gases and Liquids, | ||
227 | * 4th edition (1987, pp 396-397) \cite reid1987 <BR> | ||
228 | * 5th edition (2001, pp 9.7-9.8 (omega and V_c taken from p. A.19)) \cite poling2001 | ||
229 | * | ||
230 | */ | ||
231 | 16838318 | static Scalar gasViscosity(Scalar temperature, Scalar pressure) | |
232 | { | ||
233 | 16838318 | const Scalar Tc = criticalTemperature(); | |
234 | 16838318 | const Scalar Vc = 90.1; // critical specific volume [cm^3/mol] | |
235 | 16838318 | const Scalar omega = 0.037; // accentric factor | |
236 | 16838318 | const Scalar M = molarMass() * 1e3; // molar mas [g/mol] | |
237 | 16838318 | const Scalar dipole = 0.0; // dipole moment [debye] | |
238 | |||
239 | using std::sqrt; | ||
240 | 16838318 | Scalar mu_r4 = 131.3 * dipole / sqrt(Vc * Tc); | |
241 | 16838318 | mu_r4 *= mu_r4; | |
242 | 16838318 | mu_r4 *= mu_r4; | |
243 | |||
244 | using std::pow; | ||
245 | using std::exp; | ||
246 | 16838318 | Scalar Fc = 1 - 0.2756*omega + 0.059035*mu_r4; | |
247 | 16838318 | Scalar Tstar = 1.2593 * temperature/Tc; | |
248 | 16838318 | Scalar Omega_v = | |
249 | 33676636 | 1.16145*pow(Tstar, -0.14874) + | |
250 | 16838318 | 0.52487*exp(- 0.77320*Tstar) + | |
251 | 16838318 | 2.16178*exp(- 2.43787*Tstar); | |
252 | 16838318 | Scalar mu = 40.785*Fc*sqrt(M*temperature)/(pow(Vc, 2./3)*Omega_v); | |
253 | |||
254 | // conversion from micro poise to Pa s | ||
255 | 16838318 | return mu/1e6 / 10; | |
256 | } | ||
257 | |||
258 | /*! | ||
259 | * \brief Thermal conductivity \f$\mathrm{[[W/(m*K)]}\f$ of nitrogen. | ||
260 | * | ||
261 | * Isobaric Properties for Nitrogen and Oxygen in: NIST Standard | ||
262 | * Reference Database Number 69, Eds. P.J. Linstrom and | ||
263 | * W.G. Mallard evaluated at p=.1 MPa, does not | ||
264 | * change dramatically with p and can be interpolated linearly with temperature | ||
265 | * | ||
266 | * \param temperature absolute temperature in \f$\mathrm{[K]}\f$ | ||
267 | * \param pressure of the phase in \f$\mathrm{[Pa]}\f$ | ||
268 | */ | ||
269 | ✗ | static Scalar gasThermalConductivity(Scalar temperature, Scalar pressure) | |
270 | { | ||
271 | 18067090 | return 6.525e-5 * (temperature - 273.15) + 0.024031; | |
272 | } | ||
273 | }; | ||
274 | |||
275 | } // end namespace Components | ||
276 | |||
277 | } // end namespace Dumux | ||
278 | |||
279 | #endif | ||
280 |