GCC Code Coverage Report


Directory: ../../../builds/dumux-repositories/
File: /builds/dumux-repositories/dumux/dumux/material/components/h2o.hh
Date: 2024-05-04 19:09:25
Exec Total Coverage
Lines: 188 194 96.9%
Functions: 20 21 95.2%
Branches: 188 384 49.0%

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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 Material properties of pure water \f$H_2O\f$.
11 */
12 #ifndef DUMUX_H2O_HH
13 #define DUMUX_H2O_HH
14
15 #include <cmath>
16 #include <cassert>
17
18 #include <dumux/nonlinear/findscalarroot.hh>
19 #include <dumux/material/idealgas.hh>
20 #include <dumux/common/exceptions.hh>
21
22 #include "iapws/common.hh"
23 #include "iapws/region1.hh"
24 #include "iapws/region2.hh"
25 #include "iapws/region4.hh"
26
27 #include <dumux/material/components/base.hh>
28 #include <dumux/material/components/liquid.hh>
29 #include <dumux/material/components/gas.hh>
30
31 namespace Dumux {
32 namespace Components {
33
34 /*!
35 * \ingroup Components
36 * \brief Material properties of pure water \f$H_2O\f$.
37 * \tparam Scalar The type used for scalar values
38 *
39 * See:
40 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
41 * 1997 for the Thermodynamic Properties of Water and Steam",
42 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
43 */
44 template <class Scalar>
45 class H2O
46 : public Components::Base<Scalar, H2O<Scalar> >
47 , public Components::Liquid<Scalar, H2O<Scalar> >
48 , public Components::Gas<Scalar, H2O<Scalar> >
49 {
50
51 using Common = IAPWS::Common<Scalar>;
52 using Region1 = IAPWS::Region1<Scalar>;
53 using Region2 = IAPWS::Region2<Scalar>;
54 using Region4 = IAPWS::Region4<Scalar>;
55
56 // specific gas constant of water
57 static constexpr Scalar Rs = Common::Rs;
58
59 public:
60 /*!
61 * \brief A human readable name for the water.
62 */
63 static std::string name()
64
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799114 { return "H2O"; }
65
66 /*!
67 * \brief The molar mass in \f$\mathrm{[kg/mol]}\f$ of water.
68 */
69 static constexpr Scalar molarMass()
70 { return Common::molarMass; }
71
72 /*!
73 * \brief The acentric factor \f$\mathrm{[-]}\f$ of water.
74 */
75 static constexpr Scalar acentricFactor()
76 { return Common::acentricFactor; }
77
78 /*!
79 * \brief Returns the critical temperature \f$\mathrm{[K]}\f$ of water
80 */
81 static constexpr Scalar criticalTemperature()
82 { return Common::criticalTemperature; }
83
84 /*!
85 * \brief Returns the critical pressure \f$\mathrm{[Pa]}\f$ of water.
86 */
87 static constexpr Scalar criticalPressure()
88 { return Common::criticalPressure; }
89
90 /*!
91 * \brief Returns the molar volume \f$\mathrm{[m^3/mol]}\f$ of water at the critical point
92 */
93 static constexpr Scalar criticalMolarVolume()
94 { return Common::criticalMolarVolume; }
95
96 /*!
97 * \brief Returns the temperature \f$\mathrm{[K]}\f$ at water's triple point.
98 */
99 static constexpr Scalar tripleTemperature()
100 { return Common::tripleTemperature; }
101
102 /*!
103 * \brief Returns the pressure \f$\mathrm{[Pa]}\f$ at water's triple point.
104 */
105 static constexpr Scalar triplePressure()
106 { return Common::triplePressure; }
107
108 /*!
109 * \brief The vapor pressure in \f$\mathrm{[Pa]}\f$ of pure water
110 * at a given temperature.
111 *
112 *\param T temperature of component in \f$\mathrm{[K]}\f$
113 *
114 * See:
115 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
116 * 1997 for the Thermodynamic Properties of Water and Steam",
117 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
118 */
119 233975438 static Scalar vaporPressure(Scalar T)
120 {
121 using std::min;
122 using std::max;
123
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233975438 T = min(T, criticalTemperature());
124
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233975438 T = max(T,tripleTemperature());
125
126 233975439 return Region4::saturationPressure(T);
127 }
128
129 /*!
130 * \brief The vapor temperature in \f$\mathrm{[K]}\f$ of pure water
131 * at a given pressure.
132 *
133 *\param pressure pressure in \f$\mathrm{[Pa]}\f$
134 *
135 * See:
136 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
137 * 1997 for the Thermodynamic Properties of Water and Steam",
138 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
139 */
140 100333 static Scalar vaporTemperature(Scalar pressure)
141 {
142 using std::min;
143 using std::max;
144
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100333 pressure = min(pressure, criticalPressure());
145
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100333 pressure = max(pressure, triplePressure());
146
147 100333 return Region4::vaporTemperature(pressure);
148 }
149
150 /*!
151 * \brief Specific enthalpy of water steam \f$\mathrm{[J/kg]}\f$.
152 *
153 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
154 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
155 *
156 * See:
157 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
158 * 1997 for the Thermodynamic Properties of Water and Steam",
159 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
160 */
161 3319615 static const Scalar gasEnthalpy(Scalar temperature,
162 Scalar pressure)
163 {
164
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6639230 Region2::checkValidityRange(temperature, pressure, "Enthalpy");
165
166 // regularization
167
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3319615 if (pressure < triplePressure() - 100) {
168 // We assume an ideal gas for low pressures to avoid the
169 // 0/0 for the gas enthalpy at very low pressures. The
170 // enthalpy of an ideal gas does not exhibit any
171 // dependence on pressure, so we can just return the
172 // specific enthalpy at the point of regularization, i.e.
173 // the triple pressure - 100Pa
174 199248 return enthalpyRegion2_(temperature, triplePressure() - 100);
175 }
176 3219991 Scalar pv = vaporPressure(temperature);
177
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3219991 if (pressure > pv) {
178 // the pressure is too high, in this case we use the slope
179 // of the enthalpy at the vapor pressure to regularize
180 677612 Scalar dh_dp =
181 1355224 Rs*temperature*
182 677612 Region2::tau(temperature)*
183 677612 Region2::dPi_dp(pv)*
184 677612 Region2::ddGamma_dTaudPi(temperature, pv);
185
186 return
187 1355224 enthalpyRegion2_(temperature, pv) +
188 677612 (pressure - pv)*dh_dp;
189 }
190
191 5084758 return enthalpyRegion2_(temperature, pressure);
192 }
193
194 /*!
195 * \brief Specific enthalpy of liquid water \f$\mathrm{[J/kg]}\f$.
196 *
197 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
198 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
199 *
200 * See:
201 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
202 * 1997 for the Thermodynamic Properties of Water and Steam",
203 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
204 */
205 4957978 static const Scalar liquidEnthalpy(Scalar temperature,
206 Scalar pressure)
207 {
208
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9915956 Region1::checkValidityRange(temperature, pressure, "Enthalpy");
209
210 // regularization
211 4957978 Scalar pv = vaporPressure(temperature);
212
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4957978 if (pressure < pv) {
213 // the pressure is too low, in this case we use the slope
214 // of the enthalpy at the vapor pressure to regularize
215 82802 Scalar dh_dp =
216 165604 Rs * temperature*
217 82802 Region1::tau(temperature)*
218 82802 Region1::dPi_dp(pv)*
219 82802 Region1::ddGamma_dTaudPi(temperature, pv);
220
221 return
222 165604 enthalpyRegion1_(temperature, pv) +
223 82802 (pressure - pv)*dh_dp;
224 }
225
226 9750352 return enthalpyRegion1_(temperature, pressure);
227 }
228
229 /*!
230 * \brief Specific isobaric heat capacity of water steam \f$\mathrm{[J/(kg*K)}\f$.
231 *
232 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
233 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
234 *
235 * See:
236 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
237 * 1997 for the Thermodynamic Properties of Water and Steam",
238 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
239 */
240 2805615 static const Scalar gasHeatCapacity(Scalar temperature,
241 Scalar pressure)
242 {
243
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5611230 Region2::checkValidityRange(temperature, pressure, "Heat capacity");
244
245 // regularization
246
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2805615 if (pressure < triplePressure() - 100) {
247 199134 return heatCap_p_Region2_(temperature, triplePressure() - 100);
248 }
249 2706048 Scalar pv = vaporPressure(temperature);
250
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2706048 if (pressure > pv) {
251 // the pressure is too high, in this case we use the heat
252 // cap at the vapor pressure to regularize
253 737020 return heatCap_p_Region2_(temperature, pv);
254 }
255 4675076 return heatCap_p_Region2_(temperature, pressure);
256 }
257
258 /*!
259 * \brief Specific isobaric heat capacity of liquid water \f$\mathrm{[J/(kg*K)]}\f$.
260 *
261 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
262 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
263 *
264 * See:
265 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
266 * 1997 for the Thermodynamic Properties of Water and Steam",
267 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
268 */
269 2805983 static const Scalar liquidHeatCapacity(Scalar temperature,
270 Scalar pressure)
271 {
272
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5611966 Region1::checkValidityRange(temperature, pressure, "Heat capacity");
273
274 // regularization
275 2805983 Scalar pv = vaporPressure(temperature);
276
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2805983 if (pressure < pv) {
277 // the pressure is too low, in this case we use the heat cap at the vapor pressure to regularize
278 165116 return heatCap_p_Region1_(temperature, pv);
279 }
280
281 5446850 return heatCap_p_Region1_(temperature, pressure);
282 }
283
284 /*!
285 * \brief Specific internal energy of liquid water \f$\mathrm{[J/kg]}\f$.
286 *
287 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
288 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
289 *
290 * See:
291 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
292 * 1997 for the Thermodynamic Properties of Water and Steam",
293 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
294 */
295 1235383 static const Scalar liquidInternalEnergy(Scalar temperature,
296 Scalar pressure)
297 {
298
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2470766 Region1::checkValidityRange(temperature, pressure, "Internal energy");
299
300 // regularization
301 1235383 Scalar pv = vaporPressure(temperature);
302
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1235383 if (pressure < pv) {
303 // the pressure is too low, in this case we use the slope
304 // of the internal energy at the vapor pressure to
305 // regularize
306
307 /*
308 // calculate the partial derivative of the internal energy
309 // to the pressure at the vapor pressure.
310 Scalar tau = Region1::tau(temperature);
311 Scalar dGamma_dPi = Region1::dGamma_dPi(temperature, pv);
312 Scalar ddGamma_dTaudPi = Region1::ddGamma_dTaudPi(temperature, pv);
313 Scalar ddGamma_ddPi = Region1::ddGamma_ddPi(temperature, pv);
314 Scalar pi = Region1::pi(pv);
315 Scalar dPi_dp = Region1::dPi_dp(pv);
316 Scalar du_dp =
317 Rs*temperature*
318 (tau*dPi_dp*ddGamma_dTaudPi + dPi_dp*dPi_dp*dGamma_dPi + pi*dPi_dp*ddGamma_ddPi);
319 */
320
321 // use a straight line for extrapolation. use forward
322 // differences to calculate the partial derivative to the
323 // pressure at the vapor pressure
324 static const Scalar eps = 1e-7;
325 217 Scalar uv = internalEnergyRegion1_(temperature, pv);
326 217 Scalar uvPEps = internalEnergyRegion1_(temperature, pv + eps);
327 217 Scalar du_dp = (uvPEps - uv)/eps;
328 217 return uv + du_dp*(pressure - pv);
329 }
330
331 1235166 return internalEnergyRegion1_(temperature, pressure);
332 }
333
334 /*!
335 * \brief Specific internal energy of steam and water vapor \f$\mathrm{[J/kg]}\f$.
336 *
337 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
338 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
339 *
340 * See:
341 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
342 * 1997 for the Thermodynamic Properties of Water and Steam",
343 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
344 */
345 205023 static Scalar gasInternalEnergy(Scalar temperature, Scalar pressure)
346 {
347
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410046 Region2::checkValidityRange(temperature, pressure, "Internal energy");
348
349 // regularization
350
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205023 if (pressure < triplePressure() - 100) {
351 // We assume an ideal gas for low pressures to avoid the
352 // 0/0 for the internal energy of gas at very low
353 // pressures. The enthalpy of an ideal gas does not
354 // exhibit any dependence on pressure, so we can just
355 // return the specific enthalpy at the point of
356 // regularization, i.e. the triple pressure - 100Pa, and
357 // subtract the work required to change the volume for an
358 // ideal gas.
359 return
360 enthalpyRegion2_(temperature, triplePressure() - 100)
361 -
362 Rs*temperature; // = p*v for an ideal gas!
363 }
364 205023 Scalar pv = vaporPressure(temperature);
365
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205023 if (pressure > pv) {
366 // the pressure is too high, in this case we use the slope
367 // of the internal energy at the vapor pressure to
368 // regularize
369
370 /*
371 // calculate the partial derivative of the internal energy
372 // to the pressure at the vapor pressure.
373 Scalar tau = Region2::tau(temperature);
374 Scalar dGamma_dPi = Region2::dGamma_dPi(temperature, pv);
375 Scalar ddGamma_dTaudPi = Region2::ddGamma_dTaudPi(temperature, pv);
376 Scalar ddGamma_ddPi = Region2::ddGamma_ddPi(temperature, pv);
377 Scalar pi = Region2::pi(pv);
378 Scalar dPi_dp = Region2::dPi_dp(pv);
379 Scalar du_dp =
380 Rs*temperature*
381 (tau*dPi_dp*ddGamma_dTaudPi + dPi_dp*dPi_dp*dGamma_dPi + pi*dPi_dp*ddGamma_ddPi);
382
383 // use a straight line for extrapolation
384 Scalar uv = internalEnergyRegion2_(temperature, pv);
385 return uv + du_dp*(pressure - pv);
386 */
387
388 // use a straight line for extrapolation. use backward
389 // differences to calculate the partial derivative to the
390 // pressure at the vapor pressure
391 static const Scalar eps = 1e-7;
392 189 Scalar uv = internalEnergyRegion2_(temperature, pv);
393 189 Scalar uvMEps = internalEnergyRegion2_(temperature, pv - eps);
394 189 Scalar du_dp = (uv - uvMEps)/eps;
395 189 return uv + du_dp*(pressure - pv);
396 }
397
398 204834 return internalEnergyRegion2_(temperature, pressure);
399 }
400
401 /*!
402 * \brief Specific isochoric heat capacity of liquid water \f$\mathrm{[J/(m^3*K)]}\f$.
403 *
404 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
405 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
406 *
407 * See:
408 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
409 * 1997 for the Thermodynamic Properties of Water and Steam",
410 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
411 */
412 static const Scalar liquidHeatCapacityConstVolume(Scalar temperature,
413 Scalar pressure)
414 {
415 Region1::checkValidityRange(temperature, pressure, "Heat capacity for a constant volume");
416
417 // regularization
418 Scalar pv = vaporPressure(temperature);
419 if (pressure < pv) {
420 // the pressure is too low, in this case we use the heat cap at the vapor pressure to regularize
421
422 return heatCap_v_Region1_(temperature, pv);
423 }
424
425 return heatCap_v_Region1_(temperature, pressure);
426 }
427
428 /*!
429 * \brief Specific isochoric heat capacity of steam and water vapor \f$\mathrm{[J/(kg*K)}\f$.
430 *
431 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
432 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
433 *
434 * See:
435 *
436 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
437 * 1997 for the Thermodynamic Properties of Water and Steam",
438 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
439 */
440 static Scalar gasHeatCapacityConstVolume(Scalar temperature, Scalar pressure)
441 {
442 Region2::checkValidityRange(temperature, pressure, "Heat capacity for a constant volume");
443
444 // regularization
445 if (pressure < triplePressure() - 100) {
446 return
447 heatCap_v_Region2_(temperature, triplePressure() - 100);
448 }
449 Scalar pv = vaporPressure(temperature);
450 if (pressure > pv) {
451 return heatCap_v_Region2_(temperature, pv);
452 }
453
454 return heatCap_v_Region2_(temperature, pressure);
455 }
456
457 /*!
458 * \brief Returns true if the gas phase is assumed to be compressible
459 */
460 static constexpr bool gasIsCompressible()
461 { return true; }
462
463 /*!
464 * \brief Returns true if the liquid phase is assumed to be compressible
465 */
466 static constexpr bool liquidIsCompressible()
467 { return true; }
468
469 /*!
470 * \brief The density of steam in \f$\mathrm{[kg/m^3]}\f$ at a given pressure and temperature.
471 *
472 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
473 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
474 *
475 * See:
476 *
477 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
478 * 1997 for the Thermodynamic Properties of Water and Steam",
479 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
480 */
481 42390275 static Scalar gasDensity(Scalar temperature, Scalar pressure)
482 {
483
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84780550 Region2::checkValidityRange(temperature, pressure, "Density");
484
485 // regularization
486
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42390275 if (pressure < triplePressure() - 100) {
487 // We assume an ideal gas for low pressures to avoid the
488 // 0/0 for the internal energy and enthalpy.
489 1505264 Scalar rho0IAPWS = 1.0/volumeRegion2_(temperature,
490 triplePressure() - 100);
491 1505264 Scalar rho0Id = IdealGas<Scalar>::density(molarMass(),
492 temperature,
493 triplePressure() - 100);
494 return
495 752632 rho0IAPWS/rho0Id *
496 752632 IdealGas<Scalar>::density(molarMass(),
497 temperature,
498 752632 pressure);
499 }
500 41637643 Scalar pv = vaporPressure(temperature);
501
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41637643 if (pressure > pv) {
502 // the pressure is too high, in this case we use the slope
503 // of the density energy at the vapor pressure to
504 // regularize
505
506 // calculate the partial derivative of the specific volume
507 // to the pressure at the vapor pressure.
508 6174092 const Scalar eps = pv*1e-8;
509 12348184 Scalar v0 = volumeRegion2_(temperature, pv);
510 12348184 Scalar v1 = volumeRegion2_(temperature, pv + eps);
511 6174092 Scalar dv_dp = (v1 - v0)/eps;
512 /*
513 Scalar pi = Region2::pi(pv);
514 Scalar dp_dPi = Region2::dp_dPi(pv);
515 Scalar dGamma_dPi = Region2::dGamma_dPi(temperature, pv);
516 Scalar ddGamma_ddPi = Region2::ddGamma_ddPi(temperature, pv);
517
518 Scalar RT = Rs*temperature;
519 Scalar dv_dp =
520 RT/(dp_dPi*pv)
521 *
522 (dGamma_dPi + pi*ddGamma_ddPi - v0*dp_dPi/RT);
523 */
524
525 // calculate the partial derivative of the density to the
526 // pressure at vapor pressure
527 6174092 Scalar drho_dp = - 1/(v0*v0)*dv_dp;
528
529 // use a straight line for extrapolation
530 6174092 return 1.0/v0 + (pressure - pv)*drho_dp;
531 }
532
533 70927102 return 1.0/volumeRegion2_(temperature, pressure);
534 }
535
536 /*!
537 * \brief The molar density of steam in \f$\mathrm{[mol/m^3]}\f$ at a given pressure and temperature.
538 *
539 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
540 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
541 *
542 */
543 static Scalar gasMolarDensity(Scalar temperature, Scalar pressure)
544 2511728 { return gasDensity(temperature, pressure)/molarMass(); }
545
546 /*!
547 * \brief Returns true if the gas phase is assumed to be ideal
548 */
549 static constexpr bool gasIsIdeal()
550 { return false; }
551
552 /*!
553 * \brief The pressure of steam in \f$\mathrm{[Pa]}\f$ at a given density and temperature.
554 *
555 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
556 * \param density of component in \f$\mathrm{[kg/m^3]}\f$
557 *
558 * See:
559 *
560 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
561 * 1997 for the Thermodynamic Properties of Water and Steam",
562 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
563 */
564 3010232 static Scalar gasPressure(Scalar temperature, Scalar density)
565 {
566 // We use the newton method for this. For the initial value we
567 // assume steam to be an ideal gas
568 3010232 Scalar pressure = IdealGas<Scalar>::pressure(temperature, density/molarMass());
569 3010232 Scalar eps = pressure*1e-7;
570
571 3010232 Scalar deltaP = pressure*2;
572 using std::abs;
573
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12204329 for (int i = 0; i < 5 && abs(pressure*1e-9) < abs(deltaP); ++i)
574 {
575 9194097 const Scalar f = gasDensity(temperature, pressure) - density;
576
577 Scalar df_dp;
578 9194097 df_dp = gasDensity(temperature, pressure + eps);
579 9194097 df_dp -= gasDensity(temperature, pressure - eps);
580 9194097 df_dp /= 2*eps;
581
582 9194097 deltaP = - f/df_dp;
583
584 9194097 pressure += deltaP;
585 }
586
587 3010232 return pressure;
588 }
589
590 /*!
591 * \brief The density of pure water in \f$\mathrm{[kg/m^3]}\f$ at a given pressure and temperature.
592 *
593 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
594 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
595 *
596 * See:
597 *
598 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
599 * 1997 for the Thermodynamic Properties of Water and Steam",
600 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
601 */
602 146677879 static Scalar liquidDensity(Scalar temperature, Scalar pressure)
603 {
604
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293355758 Region1::checkValidityRange(temperature, pressure, "Density");
605
606 // regularization
607 146677873 Scalar pv = vaporPressure(temperature);
608
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146677873 if (pressure < pv) {
609 // the pressure is too low, in this case we use the slope
610 // of the density at the vapor pressure to regularize
611
612 // calculate the partial derivative of the specific volume
613 // to the pressure at the vapor pressure.
614 7828405 const Scalar eps = pv*1e-8;
615 15656810 Scalar v0 = volumeRegion1_(temperature, pv);
616 15656810 Scalar v1 = volumeRegion1_(temperature, pv + eps);
617 7828405 Scalar dv_dp = (v1 - v0)/eps;
618
619 /*
620 Scalar v0 = volumeRegion1_(temperature, pv);
621 Scalar pi = Region1::pi(pv);
622 Scalar dp_dPi = Region1::dp_dPi(pv);
623 Scalar dGamma_dPi = Region1::dGamma_dPi(temperature, pv);
624 Scalar ddGamma_ddPi = Region1::ddGamma_ddPi(temperature, pv);
625
626 Scalar RT = Rs*temperature;
627 Scalar dv_dp =
628 RT/(dp_dPi*pv)
629 *
630 (dGamma_dPi + pi*ddGamma_ddPi - v0*dp_dPi/RT);
631 */
632
633 // calculate the partial derivative of the density to the
634 // pressure at vapor pressure
635 7828405 Scalar drho_dp = - 1/(v0*v0)*dv_dp;
636
637 // use a straight line for extrapolation
638 7828405 return 1.0/v0 + (pressure - pv)*drho_dp;
639 }
640
641 277698936 return 1/volumeRegion1_(temperature, pressure);
642 }
643
644 /*!
645 * \brief The molar density of water in \f$\mathrm{[mol/m^3]}\f$ at a given pressure and temperature.
646 *
647 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
648 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
649 *
650 */
651 static Scalar liquidMolarDensity(Scalar temperature, Scalar pressure)
652 14 { return liquidDensity(temperature, pressure)/molarMass(); }
653
654 /*!
655 * \brief The pressure of liquid water in \f$\mathrm{[Pa]}\f$ at a given density and
656 * temperature.
657 *
658 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
659 * \param density density of component in \f$\mathrm{[kg/m^3]}\f$
660 *
661 * See:
662 *
663 * IAPWS: "Revised Release on the IAPWS Industrial Formulation
664 * 1997 for the Thermodynamic Properties of Water and Steam",
665 * http://www.iapws.org/relguide/IF97-Rev.pdf \cite IAPWS1997
666 */
667 4040592 static Scalar liquidPressure(Scalar temperature, Scalar density)
668 {
669 // We use Brent's method for this, with a pressure range including the surroundings of the
670 // vapor pressure line
671 4040592 Scalar minPressure = vaporPressure(temperature)/1.11;
672 4040592 Scalar maxPressure = 100e6;
673 4040592 const auto residualFunction = [&] (const Scalar pressure) {
674
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123394862 return liquidDensity(temperature, pressure) - density;
675 };
676 try
677 {
678
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4040592 return findScalarRootBrent(minPressure, maxPressure, residualFunction);
679 }
680 catch (const NumericalProblem& e)
681 {
682 DUNE_THROW(NumericalProblem,
683 "searched for pressure(T=" << temperature << ",rho=" << density
684 <<") in [" << minPressure << ", " << maxPressure << "]: "
685 << e.what());
686 }
687 }
688
689 /*!
690 * \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of steam.
691 *
692 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
693 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
694 *
695 * We assume pure water vapor here. For water in a mixture of other gaseous
696 * components, consider the free function h2oGasViscosityInMixture.
697 *
698 * We use the IAPWS Formulation, see:
699 * IAPWS: "Release on the IAPWS Formulation 2008 for the Viscosity
700 * of Ordinary Water Substance", http://www.iapws.org/relguide/visc.pdf \cite cooper2008
701 * This method is only valid if pressure is below or at the vapor
702 * pressure of water.
703 */
704 3010440 static Scalar gasViscosity(Scalar temperature, Scalar pressure)
705 {
706
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6020880 Region2::checkValidityRange(temperature, pressure, "Viscosity");
707
708 3010440 Scalar rho = gasDensity(temperature, pressure);
709 3010440 return Common::viscosity(temperature, rho);
710 }
711
712
713 /*!
714 * \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of pure water.
715 *
716 * \param temperature temperature of component in \f$\mathrm{[K]}\f$
717 * \param pressure pressure of component in \f$\mathrm{[Pa]}\f$
718 *
719 * See:
720 * IAPWS: "Release on the IAPWS Formulation 2008 for the Viscosity
721 * of Ordinary Water Substance", http://www.iapws.org/relguide/visc.pdf \cite cooper2008
722 */
723 4988805 static Scalar liquidViscosity(Scalar temperature, Scalar pressure)
724 {
725
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9977610 Region1::checkValidityRange(temperature, pressure, "Viscosity");
726
727 4988805 Scalar rho = liquidDensity(temperature, pressure);
728 4988805 return Common::viscosity(temperature, rho);
729 }
730
731 /*!
732 * \brief Thermal conductivity \f$\mathrm{[[W/(m*K)]}\f$ of water (IAPWS) .
733 *
734 * Implementation taken from:
735 * freesteam - IAPWS-IF97 steam tables library
736 * copyright (C) 2004-2009 John Pye
737 *
738 * See:
739 * IAPWS: "Release on the IAPWS Formulation 2011 for the Thermal Conductivity
740 * of Ordinary Water Substance", http://www.iapws.org/relguide/ThCond.pdf
741 * \cite IAPWS_ThCond
742 *
743 * \param temperature absolute temperature in \f$\mathrm{[K]}\f$
744 * \param pressure of the phase in \f$\mathrm{[Pa]}\f$
745 */
746 3696987 static Scalar liquidThermalConductivity( Scalar temperature, Scalar pressure)
747 {
748 // Thermal conductivity of water is empirically fit.
749 // Evaluating that fitting-function outside the area of validity does not make sense.
750
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3697004 if ( !( (pressure <= 400e6 && (273.15 <= temperature) && (temperature <= 398.15))
751
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1645217 || (pressure <= 200e6 && (398.15 < temperature) && (temperature <= 523.15))
752
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739017 || (pressure <= 150e6 && (523.15 < temperature) && (temperature <= 673.15))
753
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17 || (pressure <= 100e6 && (673.15 < temperature) && (temperature <= 1073.15)) ))
754 {
755
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204 DUNE_THROW(NumericalProblem,
756 "Evaluating the IAPWS fit function for thermal conductivity outside range of applicability."
757 "(T=" << temperature << ", p=" << pressure << ")");
758 }
759
760 3696970 Scalar rho = liquidDensity(temperature, pressure);
761 3696970 return Common::thermalConductivityIAPWS(temperature, rho);
762 }
763
764 /*!
765 * \brief Thermal conductivity \f$\mathrm{[[W/(m*K)]}\f$ of steam (IAPWS) .
766 *
767 * Implementation taken from:
768 * freesteam - IAPWS-IF97 steam tables library
769 * copyright (C) 2004-2009 John Pye
770 *
771 * See:
772 * IAPWS: "Release on the IAPWS Formulation 2011 for the Thermal Conductivity
773 * of Ordinary Water Substance", http://www.iapws.org/relguide/ThCond.pdf
774 * \cite IAPWS_ThCond
775 *
776 * \param temperature absolute temperature in \f$\mathrm{[K]}\f$
777 * \param pressure of the phase in \f$\mathrm{[Pa]}\f$
778 */
779 3047980 static Scalar gasThermalConductivity(const Scalar temperature, const Scalar pressure)
780 {
781 // Thermal conductivity of water is empirically fit.
782 // Evaluating that fitting-function outside the area of validity does not make sense.
783
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3047980 if ( !( (pressure <= 400e6 && (273.15 <= temperature) && (temperature <= 398.15))
784
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1645200 || (pressure <= 200e6 && (398.15 < temperature) && (temperature <= 523.15))
785
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739000 || (pressure <= 150e6 && (523.15 < temperature) && (temperature <= 673.15))
786 || (pressure <= 100e6 && (673.15 < temperature) && (temperature <= 1073.15)) ))
787 {
788 DUNE_THROW(NumericalProblem,
789 "Evaluating the IAPWS fit function for thermal conductivity outside range of applicability."
790 "(T=" << temperature << ", p=" << pressure << ")");
791 }
792
793 3047980 Scalar rho = gasDensity(temperature, pressure);
794 3047980 return Common::thermalConductivityIAPWS(temperature, rho);
795 }
796
797 private:
798 // the unregularized specific enthalpy for liquid water
799 static constexpr Scalar enthalpyRegion1_(Scalar temperature, Scalar pressure)
800 {
801 return
802 4875176 Region1::tau(temperature) *
803 4957978 Region1::dGamma_dTau(temperature, pressure) *
804 4957978 Rs*temperature;
805 }
806
807 // the unregularized specific isobaric heat capacity
808 static constexpr Scalar heatCap_p_Region1_(Scalar temperature, Scalar pressure)
809 {
810 return
811 2805983 - Region1::tau(temperature) * Region1::tau(temperature) *
812 2805983 Region1::ddGamma_ddTau(temperature, pressure) *
813 2805983 Rs;
814 }
815
816 // the unregularized specific isochoric heat capacity
817 static Scalar heatCap_v_Region1_(Scalar temperature, Scalar pressure)
818 {
819 Scalar tau = Region1::tau(temperature);
820 Scalar num = Region1::dGamma_dPi(temperature, pressure) - tau * Region1::ddGamma_dTaudPi(temperature, pressure);
821 Scalar diff = num * num / Region1::ddGamma_ddPi(temperature, pressure);
822
823 return
824 - tau * tau *
825 Region1::ddGamma_ddTau(temperature, pressure) * Rs +
826 diff;
827 }
828
829 // the unregularized specific internal energy for liquid water
830 1235600 static constexpr Scalar internalEnergyRegion1_(Scalar temperature, Scalar pressure)
831 {
832 return
833 1235600 Rs * temperature *
834 2471200 ( Region1::tau(temperature)*Region1::dGamma_dTau(temperature, pressure) -
835 2471200 Region1::pi(pressure)*Region1::dGamma_dPi(temperature, pressure));
836 }
837
838 // the unregularized specific volume for liquid water
839 static constexpr Scalar volumeRegion1_(Scalar temperature, Scalar pressure)
840 {
841 return
842 146677873 Region1::pi(pressure)*
843 146677873 Region1::dGamma_dPi(temperature, pressure) *
844 146677873 Rs * temperature / pressure;
845 }
846
847 // the unregularized specific enthalpy for steam
848 static constexpr Scalar enthalpyRegion2_(Scalar temperature, Scalar pressure)
849 {
850 return
851 2642003 Region2::tau(temperature) *
852 3319615 Region2::dGamma_dTau(temperature, pressure) *
853 3319615 Rs*temperature;
854 }
855
856 // the unregularized specific internal energy for steam
857 205212 static constexpr Scalar internalEnergyRegion2_(Scalar temperature, Scalar pressure)
858 {
859 return
860 205212 Rs * temperature *
861 410424 ( Region2::tau(temperature)*Region2::dGamma_dTau(temperature, pressure) -
862 410424 Region2::pi(pressure)*Region2::dGamma_dPi(temperature, pressure));
863 }
864
865 // the unregularized specific isobaric heat capacity
866 static constexpr Scalar heatCap_p_Region2_(Scalar temperature, Scalar pressure)
867 {
868 return
869 2805615 - Region2::tau(temperature) * Region2::tau(temperature) *
870 2805615 Region2::ddGamma_ddTau(temperature, pressure) *
871 2805615 Rs;
872 }
873
874 // the unregularized specific isochoric heat capacity
875 static Scalar heatCap_v_Region2_(Scalar temperature, Scalar pressure)
876 {
877 Scalar tau = Region2::tau(temperature);
878 Scalar pi = Region2::pi(pressure);
879 Scalar num = 1 + pi * Region2::dGamma_dPi(temperature, pressure) + tau * pi * Region2::ddGamma_dTaudPi(temperature, pressure);
880 Scalar diff = num * num / (1 - pi * pi * Region2::ddGamma_ddPi(temperature, pressure));
881 return
882 - tau * tau *
883 Region2::ddGamma_ddTau(temperature, pressure) * Rs
884 - diff;
885 }
886
887 // the unregularized specific volume for steam
888 static constexpr Scalar volumeRegion2_(Scalar temperature, Scalar pressure)
889 {
890 return
891 41637643 Region2::pi(pressure)*
892 42390275 Region2::dGamma_dPi(temperature, pressure) *
893 42390275 Rs * temperature / pressure;
894 }
895 };
896
897 template <class Scalar>
898 struct IsAqueous<H2O<Scalar>> : public std::true_type {};
899
900 } // end namespace Components
901
902 namespace FluidSystems::Detail {
903 // viscosity according to Reid, R.C.
904 template <class Scalar>
905 59774392 Scalar viscosityReid_(Scalar temperature)
906 {
907 59774392 constexpr Scalar tc = 647.3;
908 using std::max;
909
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59774392 const Scalar tr = max(temperature/tc, 1e-8);
910
911 59774392 const Scalar fp0 = 1.0 + 0.221*(0.96 + 0.1*(tr - 0.7));
912 59774392 constexpr Scalar xi = 3.334e-3;
913 using std::pow;
914 using std::exp;
915 119548784 const Scalar eta_xi = (0.807*pow(tr, 0.618) - 0.357*exp((-0.449)*tr)
916 59774392 + 0.34*exp((-4.058)*tr) + 0.018)*fp0;
917
918 59774392 return 1.0e-7*eta_xi/xi;
919 }
920
921 // viscosity according to Nagel, T. et al.
922 template <class Scalar>
923 Scalar viscosityNagel_(Scalar temperature)
924 {
925 25428 constexpr Scalar a1 = -4.4189440e-6;
926 25428 constexpr Scalar a2 = 4.6876380e-8;
927 25428 constexpr Scalar a3 = -5.3894310e-12;
928 25428 constexpr Scalar a4 = 3.2028560e-16;
929 25428 constexpr Scalar a5 = 4.9191790e-22;
930
931 25428 return a1 + a2*temperature + a3*temperature*temperature
932 25428 + a4*temperature*temperature*temperature
933 25428 + a5*temperature*temperature*temperature*temperature;
934 }
935 } // end FluidSystems::Detail
936 namespace FluidSystems {
937 /*!
938 * \brief The dynamic viscosity \f$\mathrm{[Pa*s]}\f$ of steam in a gas mixture.
939 *
940 * \param temperature temperature in \f$\mathrm{[K]}\f$
941 * \param pressure pressure
942 *
943 * We assume here that water is in mixture with other gaseous components.
944 * For pure water, use the gasViscosity function of Components::H2O.
945 *
946 * We apply two different laws depending on the gas temperature.
947 *
948 * For temperatures below 480 K see:
949 * "Reid, R.C., Prausnitz, J.M., Poling, B.E.: The Properties of
950 * Gases and Liquids (1987)"
951 * Lucas corresponding states method
952 * https://www.osti.gov/scitech/biblio/6504847 \cite reid1987
953 *
954 * For temperatures above 500 K see:
955 * Nagel, T. et al.: THC-Processes (2018)
956 * https://doi.org/10.1007/978-3-319-68225-9_12
957 *
958 * In the range 480 - 500 K, we interpolate between the two laws.
959 */
960 template <class Scalar>
961 59799726 Scalar h2oGasViscosityInMixture(Scalar temperature, Scalar pressure)
962 {
963
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59799726 if (temperature < 480.0)
964 59774298 return Detail::viscosityReid_(temperature);
965
966
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25428 else if (temperature > 500.0)
967 25334 return Detail::viscosityNagel_(temperature);
968
969 else // interpolate
970 {
971 94 const Scalar op = (500.0 - temperature)/20.0;
972
973 94 return op*Detail::viscosityReid_(temperature)
974 94 + (1.0 - op)*Detail::viscosityNagel_(temperature);
975 }
976 }
977 } // end namespace FluidSystems
978 } // end namespace Dumux
979
980 #endif
981