1 |
/* ASCEND modelling environment |
2 |
Copyright (C) 2006 Carnegie Mellon University |
3 |
|
4 |
This program is free software; you can redistribute it and/or modify |
5 |
it under the terms of the GNU General Public License as published by |
6 |
the Free Software Foundation; either version 2, or (at your option) |
7 |
any later version. |
8 |
|
9 |
This program is distributed in the hope that it will be useful, |
10 |
but WITHOUT ANY WARRANTY; without even the implied warranty of |
11 |
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the |
12 |
GNU General Public License for more details. |
13 |
|
14 |
You should have received a copy of the GNU General Public License |
15 |
along with this program; if not, write to the Free Software |
16 |
Foundation, Inc., 59 Temple Place - Suite 330, |
17 |
Boston, MA 02111-1307, USA. |
18 |
*//** @file |
19 |
Implementation of the reduced molar Helmholtz free energy equation of state. |
20 |
|
21 |
For nomenclature see Tillner-Roth, Harms-Watzenberg and Baehr, Eine neue |
22 |
Fundamentalgleichung f端r Ammoniak. |
23 |
|
24 |
John Pye, 29 Jul 2008. |
25 |
*/ |
26 |
|
27 |
#include <math.h> |
28 |
|
29 |
#include "helmholtz.h" |
30 |
|
31 |
/* forward decls */ |
32 |
|
33 |
static double helm_ideal(double tau, double delta, HelmholtzData *data); |
34 |
static double helm_ideal_tau(double tau, double delta, HelmholtzData *data); |
35 |
static double helm_resid(double tau, double delta, HelmholtzData *data); |
36 |
static double helm_resid_del(double tau, double delta, HelmholtzData *data); |
37 |
static double helm_resid_tau(double tau, double delta, HelmholtzData *data); |
38 |
|
39 |
/** |
40 |
Function to calculate pressure from Helmholtz free energy EOS, given temperature |
41 |
and mass density. |
42 |
|
43 |
@param T temperature in K |
44 |
@param rho mass density in kg/m続 |
45 |
@return pressure in Pa??? |
46 |
*/ |
47 |
double helmholtz_p(double T, double rho, HelmholtzData *data){ |
48 |
|
49 |
double tau = data->T_star / T; |
50 |
double delta = rho / data->rho_star; |
51 |
|
52 |
return data->R * T * rho * (1. + delta * helm_resid_del(tau,delta,data)); |
53 |
} |
54 |
|
55 |
/** |
56 |
Function to calculate internal energy from Helmholtz free energy EOS, given |
57 |
temperature and mass density. |
58 |
|
59 |
@param T temperature in K |
60 |
@param rho mass density in kg/m続 |
61 |
@return internal energy in ??? |
62 |
*/ |
63 |
double helmholtz_u(double T, double rho, HelmholtzData *data){ |
64 |
|
65 |
double tau = data->T_star / T; |
66 |
double delta = rho / data->rho_star; |
67 |
|
68 |
return data->R * T * tau * (helm_ideal_tau(tau,delta,data) + helm_resid_tau(tau,delta,data)); |
69 |
} |
70 |
|
71 |
/** |
72 |
Function to calculate enthalpy from Helmholtz free energy EOS, given |
73 |
temperature and mass density. |
74 |
|
75 |
@param T temperature in K |
76 |
@param rho mass density in kg/m続 |
77 |
@return enthalpy in ???? |
78 |
*/ |
79 |
double helmholtz_h(double T, double rho, HelmholtzData *data){ |
80 |
|
81 |
double tau = data->T_star / T; |
82 |
double delta = rho / data->rho_star; |
83 |
|
84 |
return data->R * T * (1 + tau * (helm_ideal_tau(tau,delta,data) + helm_resid_tau(tau,delta,data)) + delta*helm_resid_del(tau,delta,data)); |
85 |
} |
86 |
|
87 |
/*--------------------------------------------- |
88 |
IDEAL COMPONENT RELATIONS |
89 |
*/ |
90 |
|
91 |
/** |
92 |
Ideal component of helmholtz function |
93 |
*/ |
94 |
double helm_ideal(double tau, double delta, HelmholtzData *data){ |
95 |
double *a0; |
96 |
|
97 |
double tau13 = pow(tau,1./3.); |
98 |
double taum32 = pow(tau,-3./2.); |
99 |
double taum74 = pow(tau,-7./4.); |
100 |
|
101 |
a0 = &(data->a0[0]); |
102 |
return log(delta) + a0[0] + a0[1] * tau - log(tau) + a0[2] * tau13 + a0[3] * taum32 + a0[4] * taum74; |
103 |
} |
104 |
|
105 |
/** |
106 |
Partial dervivative of ideal component of helmholtz residual function with |
107 |
respect to tau. |
108 |
*/ |
109 |
double helm_ideal_tau(double tau, double delta, HelmholtzData *data){ |
110 |
double *a0; |
111 |
|
112 |
double taum114 = pow(tau,-11./4.); |
113 |
double taum74 = tau * taum114; |
114 |
double taum23 = pow(tau,-2./3.); |
115 |
|
116 |
a0 = &(data->a0[0]); |
117 |
|
118 |
return a0[1] - 1./tau + a0[2]/3.* taum23 - a0[3] * 3./4. * taum74 - a0[4] * 7./4. * taum114; |
119 |
} |
120 |
|
121 |
/** |
122 |
Residual part of helmholtz function. Note: we have NOT prematurely |
123 |
optimised here ;-) |
124 |
*/ |
125 |
double helm_resid(double tau, double delta, HelmholtzData *data){ |
126 |
|
127 |
double sum; |
128 |
double phir = 0; |
129 |
unsigned i; |
130 |
|
131 |
HelmholtzATD *atd = &(data->atd[0]); |
132 |
|
133 |
for(i=0; i<5; ++i){ |
134 |
phir += atd->a * pow(tau, atd->t) * pow(delta, atd->d); |
135 |
++atd; |
136 |
} |
137 |
|
138 |
sum = 0; |
139 |
for(i=5; i<10; ++i){ |
140 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d); |
141 |
++atd; |
142 |
} |
143 |
phir += exp(-delta) * sum; |
144 |
|
145 |
sum = 0; |
146 |
for(i=10; i<17; ++i){ |
147 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d); |
148 |
++atd; |
149 |
} |
150 |
phir += exp(-delta*delta) * sum; |
151 |
|
152 |
sum = 0; |
153 |
for(i=17; i<21; ++i){ |
154 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d); |
155 |
++atd; |
156 |
} |
157 |
phir += exp(-delta*delta*delta) * sum; |
158 |
|
159 |
return phir; |
160 |
} |
161 |
|
162 |
/** |
163 |
Derivative of the helmholtz residual function with respect to |
164 |
delta. |
165 |
*/ |
166 |
double helm_resid_del(double tau,double delta,HelmholtzData *data){ |
167 |
|
168 |
double sum; |
169 |
double phir = 0; |
170 |
unsigned i; |
171 |
double XdelX; |
172 |
|
173 |
HelmholtzATD *atd = &(data->atd[0]); |
174 |
|
175 |
for(i=0; i<5; ++i){ |
176 |
phir += atd->a * pow(tau, atd->t) * pow(delta, atd->d - 1) * atd->d; |
177 |
++atd; |
178 |
} |
179 |
|
180 |
sum = 0; |
181 |
XdelX = delta; |
182 |
for(i=5; i<10; ++i){ |
183 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d) * (atd->d - XdelX); |
184 |
} |
185 |
phir += exp(-delta) * sum; |
186 |
|
187 |
sum = 0; |
188 |
XdelX = 2*delta*delta; |
189 |
for(i=10; i<17; ++i){ |
190 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d) * (atd->d - XdelX); |
191 |
} |
192 |
phir += exp(-delta*delta) * sum; |
193 |
|
194 |
sum = 0; |
195 |
XdelX = 3*delta*delta*delta; |
196 |
for(i=17; i<21; ++i){ |
197 |
sum += atd->a * pow(tau, atd->t) * pow(delta, atd->d) * (atd->d - XdelX); |
198 |
} |
199 |
phir += exp(-delta*delta*delta) * sum; |
200 |
|
201 |
return phir; |
202 |
} |
203 |
|
204 |
/** |
205 |
Derivative of the helmholtz residual function with respect to |
206 |
tau. |
207 |
*/ |
208 |
double helm_resid_tau(double tau,double delta,HelmholtzData *data){ |
209 |
|
210 |
double sum; |
211 |
double phir = 0; |
212 |
unsigned i; |
213 |
|
214 |
HelmholtzATD *atd = &(data->atd[0]); |
215 |
|
216 |
for(i=0; i<5; ++i){ |
217 |
if(atd->t != 0){ |
218 |
phir += atd->a * pow(tau, atd->t - 1) * pow(delta, atd->d) * atd->t; |
219 |
} |
220 |
++atd; |
221 |
} |
222 |
|
223 |
sum = 0; |
224 |
for(i=5; i<10; ++i){ |
225 |
if(atd->t != 0){ |
226 |
sum += atd->a * pow(tau, atd->t - 1) * pow(delta, atd->d) * atd->t; |
227 |
} |
228 |
++atd; |
229 |
} |
230 |
phir += exp(-delta) * sum; |
231 |
|
232 |
sum = 0; |
233 |
for(i=10; i<17; ++i){ |
234 |
if(atd->t != 0){ |
235 |
sum += atd->a * pow(tau, atd->t - 1) * pow(delta, atd->d) * atd->t; |
236 |
} |
237 |
++atd; |
238 |
} |
239 |
phir += exp(-delta*delta) * sum; |
240 |
|
241 |
sum = 0; |
242 |
for(i=17; i<21; ++i){ |
243 |
if(atd->t != 0){ |
244 |
sum += atd->a * pow(tau, atd->t - 1) * pow(delta, atd->d) * atd->t; |
245 |
} |
246 |
++atd; |
247 |
} |
248 |
phir += exp(-delta*delta*delta) * sum; |
249 |
|
250 |
return phir; |
251 |
} |
252 |
|
253 |
|
254 |
|
255 |
|