density of methanol + water between 250 k and 440 k and up to 40
DESCRIPTION
ATRANSCRIPT
-
Density of Methanol + Water between 250 K and 440 K and up to 40MPa and Vapor-Liquid Equilibria from 363 K to 440 K
Philippe Sentenac, Yves Bur, Evelyne Rauzy, and Charles Berro*
Departement de Chimie, Faculte des Sciences de Luminy, Universite de la Mediterranee,13288 Marseille Cedex 9, France
The density of methanol + water has been measured between 257.3 K and 442.15 K as a function ofpressure at five compositions by means of a high-pressure apparatus implementing a metal bellows as asimple cell. Bubble pressures have been determined at five temperatures between 363.15 K and 442.15K. They are compared with literature data that have been correlated by using the excess function-equation of state model.
Introduction
A knowledge of the thermodynamic properties of themethanol + water system is very important in order toimprove the prediction of phase equilibria. Numerousvapor-liquid equilibria, excess enthalpies, and excess vol-umes at atmospheric pressure have been measured attemperatures between 298.15 K and 333.15 K (McGlashanand Williamson, 1976; Benson and Kiyohara, 1980; Pateland Sandler, 1985). Few data exist above these temper-atures and under pressure. Excess volumes have beenreported by Easteal and Woolf (1985) between 278 K to323 K at pressures to 280 MPa and recently by Xiao et al.(1997) between 323 K and 573 K at two pressures of 7 MPaand 13.5 MPa. On the other hand, vapor-liquid equilibriahave been measured by Griswold and Wong (1952) at fourtemperatures between 373 K and 523 K, by Schroder (1958)at 413.15 K, and by Hirata and Suda (1967) and Hirata etal. (1975) at pressures of 0.3 MPa and 0.5 MPa.
In this work, densities are reported as a function ofpressure for methanol + water over a wide range oftemperature and composition. We have also determinedbubble pressures at five temperatures between 373 K and423 K.
Experimental Section
Materials. Methanol provided by Prolabo (Paris, France)had a stated minimum purity of 99%. It was purified byfractional distillation on a 60-plate Oldershaw type columnand was controlled by gas-chromatographic analysis (purity> 99.90%). The main impurity was water (
-
are carried out at given intervals of density in adjustingthe number of micrometric steps. The experiment contin-ues by decompressing the cell to the next pressure byopening and closing regulation valves (8). A measurementfor a single isotherm took 1 day.Experimental Results
Table 1 lists the density and pressure measurements ofmethanol (1) + water (2) for five compositions at ninetemperatures ranging from 257.3 K to 442.15 K. For themole fractions of methanol of 0.1061 and 0.2872, the PVTproperties have not been measured along the isotherm of257 K on account of the vicinity of melting points ofmethanol + water.
In Figure 3, the volume is plotted as a function ofpressure at constant composition (x1 ) 0.4980). The bubblepressure corresponds to the intersection of the curvesrepresenting the one-phase and two-phase regions. Thebubble pressure and composition data at five temperatures(from 363.15 K to 442.15 K) are presented in Table 2. Wehave not reported bubble pressures at lower temperaturessince the values are too small.Results and Discussion
It was difficult to compare directly our P, F, T data withthose reported in the literature since they are few innumber and are often outside the temperatures andpressures studied. Recently, Xiao et al. (1997) developeda modified corresponding-states model based on theirmeasurements and available at temperatures between 323K and 573 K and pressures between 7 MPa and 13.5 MPa.To evaluate our data, this model was used. The meanrelative deviation and the mean relative bias betweenexperimental and calculated densities defined by
are presented in Table 3. Agreement seems quite accept-able.
For vapor-liquid equilibria, the methanol + water datawere correlated using the model excess function-equationof state described previously (Peneloux et al., 1989). To
represent the properties of pure compounds a volume-translated Peng-Robinson equation of state was adopted:
The pseudo-covolume b was calculated from critical con-stants, and the dependent-temperature function a(T) isgiven by
where a(Tb) is the value of parameter a at the normalboiling temperature Tb. Parameters m1 and m2 wereadjusted in accordance with vapor pressures of purecomponents. Their values are listed in Table 4.
The excess function is defined at packing fraction ( )b/v), and the mixture equation has the following form
with
Eij denotes the binary energy parameter and varies withtemperature according to
Eij and r are two parameters adjusted using vapor-liquid equilibrium data. The isothermal VLE values be-twwen 243 K and 473 K and isobaric VLE values atatmospheric pressure reported in the literature and givenin Table 5 were selected for this evaluation. We find Eij )365.8 J cm-3 and r ) -1.823. It should be noted that wehave not taken into account our measurements in adjust-ment.
The relative mean deviation in the bubble-point pressureand absolute mean deviation in the vapor-phase composi-
Figure 1. Schematic diagram of the experimental apparatus: (1) oil tank; (2) filter; (3) piston pump; (4) shock absorber; (5) pressuregauge Heise; (6) pressure gauges; (7) breaking disk; (8) regulation valves; (9) micrometric table; (10) platinum resistance thermometer;(11) thermic regulation; (12) product introduction valve; (13) climatic fence; (14) autoclave and bellows; (15) filling cell; (16) vacuumpump.
F/F(%) )100
Ni)1
N
jFexp,i - Fcal,i
Fexp,ij (1)
r(F) )100
Ni)1
N Fexp,i - Fcal,i
Fexp,i(2)
P ) RTv - b
-a(T)
v(v + b)with ) 2(x2 + 1) (3)
a(T) ) a(Tb){1 + m1[1 - ( TTb)0.05] - m2(1 - TTb)} (4)
z )1
1 - -
i)1
p xiai
RTbiQ() +
1
2i)1
p
j)1
p b ib jxixj
i)1
p
xib i
Eij(T)
RTQ()
(5)
Q() ) 1 +
Eij ) Eij(TT )r
T ) 298.15 K (6)
Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998 593
-
Tab
le1.
P,G
Dat
afo
rM
eth
anol
(1)
+W
ater
(2)
atD
iffe
ren
tT
emp
erat
ure
s
P/M
Pa
F/m
oL-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF
/moL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
x 1)
0.10
61T
)27
2.46
KT
)30
2.60
KT
)33
2.55
KT
)36
3.17
KT
)38
3.57
KT
)40
3.52
KT
)42
4.05
KT
)44
3.49
K17
.355
52.3
000
40.1
4551
.451
437
.121
49.0
102
40.5
2347
.556
029
.198
45.6
890
37.8
3745
.027
028
.986
43.4
205
28.5
1942
.300
815
.863
52.2
032
38.7
4651
.354
435
.653
48.9
295
39.1
0447
.476
427
.703
45.6
076
36.3
5644
.951
727
.598
43.3
495
27.0
8142
.232
414
.346
52.1
246
37.2
6951
.279
934
.171
48.8
406
37.5
3847
.385
526
.201
45.5
273
34.8
5344
.880
626
.151
43.2
738
25.6
2742
.167
812
.905
52.0
356
35.8
1551
.190
432
.735
48.7
498
36.0
5247
.309
024
.723
45.4
574
33.3
3444
.803
224
.659
43.1
963
24.1
5242
.099
311
.482
51.9
425
34.3
4851
.107
231
.233
48.6
613
34.5
4847
.225
023
.272
45.3
919
31.8
2644
.724
723
.158
43.1
320
22.7
0142
.033
79.
949
51.8
667
32.8
2751
.024
929
.745
48.5
769
33.0
4947
.138
221
.813
45.3
292
30.3
3344
.644
521
.773
43.0
586
21.2
9341
.975
18.
476
51.7
925
31.3
3750
.937
528
.268
48.4
973
31.5
6547
.047
320
.441
45.2
438
28.9
0544
.561
620
.368
42.9
806
19.8
8841
.918
27.
021
51.7
151
29.8
4750
.840
026
.757
48.4
252
30.0
2546
.968
919
.079
45.1
697
27.4
9444
.483
518
.902
42.9
089
18.3
5841
.844
45.
601
51.6
315
28.3
9150
.744
825
.266
48.3
427
28.5
0946
.883
117
.598
45.0
952
26.1
2244
.402
417
.362
42.8
359
16.8
8441
.773
34.
077
51.5
441
27.0
4350
.664
923
.902
48.2
615
26.9
9746
.802
116
.131
45.0
165
24.6
9444
.327
315
.842
42.7
695
15.3
8141
.703
12.
596
51.4
678
25.5
1150
.590
022
.435
48.1
765
25.5
3446
.725
414
.686
44.9
455
23.1
8344
.258
914
.343
42.7
096
13.9
4441
.634
41.
128
51.3
988
24.0
2950
.498
321
.009
48.0
871
24.0
5946
.646
813
.375
44.8
743
21.7
7444
.162
612
.937
42.6
513
12.4
9441
.576
622
.501
50.4
026
19.5
0648
.004
822
.661
46.5
739
12.0
0544
.801
620
.292
44.0
865
11.4
0142
.586
610
.993
41.5
127
21.0
0950
.312
318
.055
47.9
235
21.2
4046
.495
010
.641
44.7
327
18.9
0744
.019
19.
926
42.5
177
9.51
641
.455
219
.582
50.2
236
16.5
8847
.850
419
.719
46.4
122
9.33
444
.655
617
.554
43.9
426
8.42
342
.462
68.
053
41.3
906
18.1
1950
.148
515
.230
47.7
787
18.3
2446
.335
57.
894
44.5
886
16.0
5143
.867
36.
935
42.3
993
6.65
841
.337
116
.682
50.0
708
13.7
5147
.700
016
.893
46.2
602
6.49
244
.525
014
.628
43.8
131
5.56
642
.337
05.
274
41.2
804
15.3
0249
.982
112
.323
47.6
207
15.4
1646
.187
65.
141
44.4
570
13.1
8843
.738
24.
134
42.2
759
3.86
441
.218
613
.828
49.8
892
10.9
3147
.538
513
.928
46.1
188
3.81
644
.400
511
.904
43.6
678
2.74
742
.217
52.
473
41.1
474
12.3
1149
.798
59.
598
47.4
634
12.3
9646
.054
22.
519
44.3
280
10.5
8543
.599
11.
199
40.9
851
1.34
237
.946
010
.808
49.7
160
8.11
347
.393
711
.049
45.9
800
1.25
544
.265
19.
110
43.5
257
0.78
437
.159
01.
193
33.4
167
9.36
749
.636
16.
712
47.3
218
9.69
545
.902
10.
464
41.6
114
7.73
043
.463
30.
732
33.7
583
1.16
629
.637
07.
985
49.5
624
5.26
947
.247
78.
275
45.8
338
0.42
339
.738
26.
379
43.3
917
0.70
829
.902
01.
177
26.7
206
6.64
849
.488
63.
889
47.1
728
6.81
745
.766
50.
318
33.8
429
5.08
243
.324
00.
679
26.9
269
1.17
324
.423
45.
206
49.4
055
2.56
447
.105
25.
382
45.6
896
0.28
729
.943
13.
734
43.2
580
0.68
124
.592
31.
159
22.5
790
3.77
749
.320
81.
206
47.0
266
3.99
445
.620
80.
255
26.9
359
2.41
643
.203
30.
669
22.7
125
1.15
521
.042
42.
456
49.2
504
2.62
445
.542
30.
239
24.5
851
1.12
343
.146
20.
646
21.1
582
1.11
119
.726
11.
087
49.1
642
1.17
245
.477
20.
228
22.6
978
0.64
037
.906
10.
660
19.8
057
1.13
218
.541
90.
303
44.0
695
0.24
320
.853
90.
548
33.5
597
0.68
218
.603
51.
140
17.4
350
0.25
441
.048
50.
238
19.5
241
0.46
329
.793
10.
624
17.4
884
1.10
516
.358
40.
211
35.4
289
0.23
018
.338
80.
495
26.8
609
0.65
416
.403
51.
123
15.2
750
0.16
631
.150
50.
215
17.2
248
0.47
524
.551
10.
655
15.3
170
1.09
214
.160
60.
183
27.8
672
0.23
116
.134
80.
473
22.6
819
0.64
814
.203
91.
077
13.0
241
0.15
024
.871
20.
224
15.0
163
0.44
921
.139
20.
619
13.0
596
0.15
922
.879
90.
210
13.8
605
0.43
719
.810
00.
153
21.2
366
0.20
812
.683
00.
420
18.6
181
0.19
119
.833
40.
440
17.5
121
0.10
418
.602
90.
397
16.4
346
0.12
517
.419
60.
382
15.3
565
0.10
816
.296
40.
421
14.2
456
0.10
715
.130
80.
382
13.1
053
594 Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998
-
Tab
le1.
(Con
tin
ued
)
P/M
Pa
F/m
oL-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF
/moL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
x 1)
0.28
72T
)27
2.36
KT
)30
2.32
KT
)33
2.81
KT
)36
3.00
KT
)38
3.52
KT
)40
3.52
KT
)42
4.29
KT
)44
2.71
K15
.193
41.8
476
27.4
4240
.985
131
.872
39.7
126
38.9
4138
.636
436
.860
37.8
328
38.8
3536
.879
538
.419
36.2
004
28.8
3135
.019
513
.663
41.7
896
25.9
7640
.922
830
.436
39.6
629
37.5
5138
.585
635
.373
37.7
823
37.2
4636
.836
536
.823
36.1
508
27.2
2034
.980
112
.207
41.7
327
24.6
1940
.806
828
.952
39.6
132
36.1
6438
.529
033
.772
37.7
319
35.6
6436
.796
335
.212
36.1
110
25.6
1734
.944
210
.736
41.6
688
23.1
1840
.747
327
.478
39.5
625
34.7
6138
.471
232
.210
37.6
796
34.1
2336
.746
233
.609
36.0
757
24.0
2934
.903
29.
232
41.6
102
21.6
4140
.692
925
.986
39.5
102
33.4
3538
.421
530
.636
37.6
331
32.5
5436
.703
432
.019
36.0
286
22.3
8434
.856
07.
776
41.5
529
20.1
2140
.625
624
.518
39.4
609
31.9
3338
.374
929
.062
37.5
788
30.9
5136
.664
330
.406
35.9
888
20.7
9534
.816
06.
350
41.4
966
18.6
8940
.588
123
.082
39.4
100
30.4
5238
.331
127
.468
37.5
256
29.4
3636
.623
528
.805
35.9
424
19.1
8834
.773
14.
877
41.4
289
17.2
8440
.530
521
.648
39.3
636
28.9
8138
.284
925
.944
37.4
716
27.9
6836
.579
827
.217
35.8
932
17.5
8434
.737
03.
501
41.3
884
15.8
5340
.474
120
.242
39.3
116
27.5
1138
.239
424
.415
37.4
260
26.4
0136
.535
925
.605
35.8
433
15.9
8634
.695
02.
114
41.3
293
14.3
8740
.423
318
.773
39.2
623
26.0
2638
.192
822
.937
37.3
874
24.8
6236
.486
924
.002
35.7
974
143.
8434
.654
71.
115
41.2
802
12.9
9340
.380
717
.287
39.2
118
24.5
5738
.145
021
.403
37.3
406
23.3
1336
.441
522
.403
35.7
543
12.7
6334
.617
711
.602
40.3
375
15.8
7639
.164
523
.080
38.0
994
19.9
4437
.289
121
.733
36.3
995
20.8
1035
.701
911
.158
34.5
818
10.1
8640
.284
314
.445
39.1
239
21.5
7938
.055
518
.401
37.2
379
20.1
6836
.353
019
.214
35.6
547
9.55
734
.542
98.
730
40.2
241
12.9
8139
.061
820
.062
38.0
077
16.8
3737
.191
018
.672
36.3
089
17.6
0635
.612
57.
940
34.5
058
7.30
640
.169
111
.503
39.0
143
18.5
7237
.961
815
.301
37.0
887
17.0
6936
.267
715
.986
35.5
683
6.30
834
.466
15.
817
40.1
209
10.0
8038
.955
417
.129
37.9
168
13.7
9737
.039
515
.488
36.2
242
14.4
1935
.527
04.
770
34.4
307
4.41
140
.070
28.
579
38.9
161
15.6
6737
.869
012
.315
36.9
894
14.0
0136
.185
112
.821
35.4
842
3.44
434
.385
63.
031
40.0
114
7.11
038
.868
714
.255
37.8
268
10.8
4136
.947
012
.426
36.1
407
11.2
1635
.437
82.
432
34.2
961
1.63
139
.958
15.
148
38.8
174
12.8
0937
.782
99.
357
36.8
991
10.9
3936
.095
19.
659
35.3
952
1.71
430
.680
01.
158
39.9
016
3.72
538
.767
311
.388
37.7
334
7.86
836
.857
59.
430
36.0
527
8.01
035
.355
71.
603
27.8
430
2.39
738
.710
39.
931
37.6
873
6.36
536
.812
57.
906
36.0
172
6.41
435
.314
71.
532
25.5
861
1.15
038
.665
08.
531
37.6
405
4.88
236
.766
36.
302
35.9
786
4.82
435
.276
91.
479
23.7
606
7.06
737
.597
63.
432
36.7
163
4.78
935
.931
23.
365
35.2
096
1.50
622
.216
25.
589
37.5
569
2.07
836
.655
23.
401
35.8
883
2.30
735
.167
71.
485
20.8
676
4.13
737
.506
40.
990
33.9
100
2.10
835
.834
51.
107
32.8
230
1.47
919
.649
22.
674
37.4
597
0.39
530
.458
00.
937
33.2
874
1.00
929
.531
11.
436
18.4
868
1.31
237
.406
80.
389
27.6
454
0.71
329
.883
60.
977
26.9
424
1.44
017
.344
60.
925
37.3
046
0.32
225
.401
40.
627
27.1
880
0.96
124
.862
21.
444
16.1
813
0.63
533
.459
70.
287
23.5
835
0.59
025
.039
10.
916
23.1
514
1.43
814
.985
80.
485
32.8
309
0.25
322
.048
60.
549
23.2
849
0.93
721
.692
51.
429
13.5
202
0.25
929
.560
00.
287
20.7
117
0.58
821
.797
30.
873
20.4
005
0.18
226
.936
70.
225
19.4
903
0.56
420
.256
50.
900
19.2
097
0.12
924
.840
70.
253
18.3
268
0.54
819
.066
80.
883
18.0
584
0.15
123
.116
70.
254
17.1
747
0.53
817
.913
50.
845
16.9
016
0.12
521
.650
90.
253
16.0
046
0.49
416
.759
70.
852
15.7
255
0.13
920
.118
30.
240
14.7
970
0.51
815
.580
90.
855
14.5
181
0.13
618
.925
20.
501
14.3
665
0.11
117
.772
30.
104
16.6
126
0.10
815
.424
60.
101
14.1
744
Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998 595
-
Tab
le1.
(Con
tin
ued
)
P/M
Pa
F/m
oL-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF
/moL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
x 1)
0.49
80T
)25
6.87
KT
)27
2.39
KT
)30
1.67
KT
)33
2.82
KT
)36
3.14
KT
)38
3.25
KT
)40
3.64
KT
)42
4.34
KT
)44
2.72
K14
.026
38.8
674
18.4
5938
.052
039
.013
37.1
646
34.1
5335
.163
839
.095
33.8
206
38.1
2832
.588
438
.223
31.6
585
34.9
5930
.660
314
.043
28.9
217
12.5
1938
.796
516
.955
37.9
798
37.6
2537
.099
332
.695
35.1
029
37.7
1633
.762
936
.775
32.5
371
36.8
5931
.604
633
.676
30.6
126
9.14
628
.732
911
.059
38.7
274
15.4
2337
.911
636
.151
37.0
413
31.1
9735
.045
836
.315
33.7
024
35.3
7232
.485
635
.446
31.5
514
32.4
1730
.565
37.
814
28.6
879
9.58
238
.663
813
.925
37.8
488
34.6
4936
.964
329
.694
34.9
800
34.9
1733
.640
833
.985
32.4
388
34.0
7731
.499
531
.136
30.5
148
6.66
328
.638
48.
049
38.5
902
12.4
5737
.780
633
.194
36.9
047
28.2
4034
.916
733
.530
33.5
839
32.6
6132
.392
532
.693
31.4
456
29.8
3930
.463
75.
353
28.5
922
6.61
438
.519
211
.021
37.7
079
31.7
9536
.845
326
.762
34.8
348
32.1
2833
.526
331
.280
32.3
444
31.2
7631
.393
028
.581
30.4
140
4.05
428
.547
05.
094
38.4
752
9.58
737
.641
130
.368
36.8
067
25.2
4934
.792
130
.690
33.4
685
29.9
2232
.299
629
.865
31.3
390
27.2
7730
.364
12.
810
28.4
974
3.73
438
.399
58.
125
37.5
677
28.8
3636
.755
723
.743
34.7
344
29.3
2633
.409
028
.520
32.2
492
28.4
9131
.290
626
.018
30.3
176
2.14
226
.816
12.
217
38.2
449
6.68
337
.499
927
.372
36.7
045
22.2
4634
.678
927
.952
33.3
488
27.1
8532
.200
327
.129
31.2
383
24.7
2330
.268
41.
881
24.4
609
5.23
037
.427
925
.940
36.5
701
20.7
6534
.619
226
.551
33.2
928
25.8
0732
.153
125
.673
31.1
875
23.4
7730
.222
91.
753
21.3
522
3.79
937
.366
224
.454
36.5
134
19.2
6134
.553
625
.172
33.2
357
24.4
0832
.104
924
.272
31.1
406
22.1
9230
.174
51.
702
18.9
826
2.36
637
.298
022
.986
36.4
423
17.7
9634
.485
523
.767
33.1
762
23.0
1932
.056
922
.894
31.0
892
20.9
1830
.130
11.
674
17.1
491
21.5
5636
.369
616
.317
34.4
238
22.4
1133
.122
121
.665
32.0
105
21.4
8731
.037
819
.650
30.0
815
1.64
315
.702
520
.104
36.2
855
14.8
1634
.361
221
.112
33.0
627
20.3
0031
.961
420
.040
30.9
907
18.3
5030
.030
71.
637
14.5
364
18.6
2536
.229
413
.319
34.3
004
19.7
1333
.007
018
.899
31.9
102
18.6
0530
.940
717
.081
29.9
833
1.63
613
.568
117
.122
36.1
654
11.8
9634
.236
618
.334
32.9
553
17.5
2031
.863
917
.208
30.8
933
15.8
3429
.935
81.
627
12.7
266
15.6
6936
.086
910
.331
34.1
786
16.9
2632
.897
316
.133
31.8
143
15.7
4330
.842
114
.599
29.8
897
1.62
211
.974
414
.199
36.0
219
8.79
934
.123
315
.539
32.8
355
14.7
2731
.771
014
.332
30.7
921
13.3
2129
.844
71.
608
11.2
704
12.7
7535
.941
97.
297
34.0
701
14.1
4832
.778
213
.349
31.7
291
12.8
9630
.746
412
.031
29.8
008
1.59
210
.583
511
.321
35.8
645
5.80
834
.010
012
.838
32.7
221
11.9
9031
.682
311
.490
30.6
988
10.7
9529
.753
71.
565
9.88
939.
842
35.7
936
4.24
533
.944
911
.443
32.6
656
10.5
8731
.636
610
.142
30.6
491
9.56
029
.705
71.
595
9.17
878.
386
35.7
277
2.86
733
.887
210
.024
32.6
064
9.29
331
.589
18.
892
30.5
996
8.29
629
.662
31.
581
8.35
846.
885
35.6
605
8.67
832
.550
27.
973
31.5
480
7.56
330
.553
27.
033
29.6
175
5.45
335
.622
57.
508
32.4
926
6.70
331
.509
56.
261
30.5
050
5.74
129
.569
54.
037
35.5
847
6.19
932
.443
65.
330
31.4
568
4.93
830
.459
84.
497
29.5
260
2.74
635
.479
74.
759
32.3
907
4.04
731
.414
43.
617
30.4
128
3.19
729
.482
33.
493
32.3
407
2.77
131
.366
22.
286
30.3
687
2.12
629
.470
52.
224
32.2
892
1.61
730
.910
11.
348
29.3
962
1.11
919
.484
61.
033
31.5
473
1.01
729
.949
51.
068
28.2
593
1.06
517
.520
40.
365
25.6
849
0.56
825
.589
10.
757
24.1
331
1.04
115
.981
00.
254
22.3
322
0.43
622
.126
70.
692
2.10
064
1.01
214
.757
20.
212
19.6
228
0.37
819
.462
30.
648
18.6
451
1.02
113
.742
80.
211
17.5
868
0.34
617
.466
00.
652
16.5
538
0.99
912
.732
10.
162
16.0
050
0.30
515
.923
60.
578
15.2
078
0.97
511
.973
40.
109
14.7
545
0.31
914
.702
40.
598
14.1
196
0.98
311
.263
10.
149
13.7
332
0.27
813
.696
60.
550
13.2
013
0.98
110
.575
40.
119
12.7
010
0.26
012
.833
20.
575
12.3
966
0.94
89.
8790
0.10
511
.929
80.
289
11.9
230
0.55
511
.661
30.
961
9.16
100.
122
11.2
172
0.27
811
.212
60.
537
10.9
647
0.94
88.
4296
0.10
710
.523
60.
276
10.5
181
0.55
110
.277
20.
109
9.68
680.
273
9.81
730.
550
9.40
030.
104
8.95
970.
265
9.09
850.
544
8.66
980.
102
8.21
970.
234
8.36
12
596 Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998
-
Tab
le1.
(Con
tin
ued
)
P/M
Pa
F/m
oL-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF
/moL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
x 1)
0.68
76T
)25
7.34
KT
)27
2.91
KT
)30
2.47
KT
)33
3.14
KT
)36
3.05
KT
)38
3.29
KT
)40
3.43
KT
)42
3.26
KT
)44
3.02
K15
.762
34.9
700
28.5
5934
.688
436
.268
33.4
872
39.6
5931
.931
438
.622
30.3
356
36.2
8129
.395
438
.996
28.6
290
38.9
3927
.855
732
.887
27.0
253
14.4
1734
.906
927
.219
34.6
306
34.9
0733
.429
438
.252
31.8
773
37.0
9130
.288
234
.687
29.3
492
37.5
4728
.586
737
.353
27.8
074
31.3
6827
.008
213
.118
34.8
471
25.8
5434
.569
833
.593
33.3
669
36.7
5731
.817
735
.568
30.2
390
33.1
2229
.301
336
.080
28.5
412
35.7
7627
.764
229
.803
26.9
544
11.8
2634
.785
224
.543
34.5
092
32.2
8333
.305
335
.269
31.7
535
34.0
8830
.188
131
.640
29.2
520
34.5
7128
.493
434
.173
27.7
152
28.2
3526
.909
110
.515
34.7
190
23.2
5334
.442
930
.958
33.2
474
33.7
0931
.703
532
.581
30.1
389
30.1
1829
.207
433
.050
28.4
487
32.5
5327
.671
726
.618
26.8
666
9.21
134
.658
221
.892
34.3
839
29.6
3533
.194
232
.254
31.6
484
31.1
1230
.087
528
.617
29.1
648
31.5
5928
.405
730
.940
27.6
239
25.0
0826
.821
37.
943
34.5
966
20.5
6734
.328
628
.328
33.1
366
30.7
8131
.588
929
.582
30.0
389
27.1
2729
.121
630
.028
28.3
661
29.3
5627
.575
823
.417
26.7
798
6.62
234
.532
619
.212
34.2
658
26.9
6333
.079
529
.367
31.5
384
28.0
3529
.994
825
.605
29.0
790
28.5
5328
.323
627
.734
27.5
290
21.8
3026
.735
55.
372
34.4
651
17.9
1034
.205
425
.641
33.0
214
27.8
9831
.481
026
.534
29.9
406
24.1
1029
.034
627
.063
28.2
795
26.0
9327
.486
520
.283
26.6
942
4.03
234
.409
916
.576
34.1
419
24.3
2132
.958
826
.367
31.4
269
25.0
7029
.901
222
.607
28.9
929
25.5
4928
.236
724
.482
27.4
429
18.6
4626
.654
32.
698
34.3
496
15.1
9934
.081
522
.980
32.9
045
24.9
0131
.374
823
.531
29.8
579
21.1
1928
.955
124
.027
28.1
954
22.8
5827
.396
417
.142
26.6
085
1.45
734
.300
713
.902
34.0
206
21.6
1632
.849
023
.377
31.3
181
22.0
2029
.804
119
.632
28.9
112
22.5
5328
.148
821
.260
27.3
533
15.5
8126
.566
412
.591
33.9
614
20.3
1232
.791
321
.887
31.2
642
20.5
4929
.755
118
.120
28.8
646
20.9
8928
.103
019
.655
27.3
067
13.9
7226
.525
611
2.88
33.8
974
18.9
8032
.731
820
.422
31.2
054
19.0
6329
.716
316
.606
28.8
186
19.4
6828
.058
618
.061
27.2
657
12.3
2726
.481
29.
820
33.8
389
17.6
2032
.675
118
.889
31.1
443
17.5
6029
.674
415
.086
28.7
718
17.9
6528
.018
116
.494
27.2
236
10.7
4026
.439
08.
466
33.7
841
16.3
1432
.614
517
.391
31.0
856
16.0
6529
.631
913
.563
28.7
262
16.5
2627
.976
814
.871
27.1
775
9.20
626
.402
17.
141
33.7
242
14.9
9032
.555
015
.913
31.0
288
14.5
2629
.593
512
.029
28.6
840
15.0
1927
.936
313
.240
27.1
400
7.47
526
.362
05.
905
33.6
610
13.6
8532
.499
714
.426
30.9
751
13.0
5229
.549
810
.526
28.6
391
13.4
8627
.892
911
.654
27.1
069
5.84
826
.323
04.
550
33.5
964
12.3
2232
.442
913
.020
30.9
214
11.5
4529
.499
29.
045
28.5
980
11.9
9927
.853
19.
975
27.0
647
4.30
026
.278
33.
264
33.5
380
10.6
7532
.386
011
.593
30.8
667
10.0
2429
.450
97.
513
28.5
532
10.5
3327
.811
08.
345
27.0
198
2.78
326
.238
81.
900
33.4
853
9.66
432
.273
410
.137
30.8
165
8.53
929
.408
85.
985
28.5
116
9.06
027
.772
06.
834
26.9
785
1.93
621
.329
41.
172
33.4
260
8.34
032
.225
58.
540
30.7
640
7.04
729
.369
64.
459
28.4
654
7.63
627
.727
05.
295
26.9
332
1.92
218
.887
67.
015
32.1
692
6.94
730
.707
95.
537
29.3
253
3.11
028
.417
46.
040
27.6
846
4.85
226
.895
61.
876
16.9
983
5.63
732
.111
65.
488
30.6
633
4.34
529
.282
81.
731
28.3
720
4.58
427
.647
22.
549
26.8
507
1.91
315
.512
44.
316
32.0
516
4.12
830
.611
52.
634
29.2
301
0.99
528
.330
93.
104
27.6
020
1.33
225
.454
51.
855
14.3
215
2.93
832
.002
72.
753
30.5
616
1.19
729
.187
10.
391
24.3
320
1.77
227
.559
51.
264
23.1
957
1.86
513
.337
91.
688
31.9
490
1.42
030
.521
21.
061
29.1
560
0.38
821
.025
70.
942
27.5
290
1.19
320
.316
31.
879
12.4
982
0.32
925
.623
70.
385
18.6
454
0.70
523
.336
31.
169
18.1
122
1.85
711
.753
50.
280
22.2
194
0.38
717
.195
80.
695
20.1
435
1.18
316
.399
91.
854
11.0
627
0.22
519
.606
20.
380
15.4
494
0.69
217
.643
11.
203
15.0
410
1.88
610
.265
50.
255
17.2
365
0.36
914
.264
80.
729
16.0
273
1.18
813
.936
81.
837
9.59
750.
209
15.7
073
0.38
113
.285
50.
698
14.7
389
1.14
713
.012
01.
859
8.91
220.
206
14.4
824
0.39
212
.448
90.
691
13.6
819
1.19
212
.212
01.
872
8.20
960.
180
13.4
720
0.34
711
.706
60.
681
12.7
947
1.16
611
.485
90.
167
12.6
137
0.37
611
.014
30.
693
12.0
167
1.18
810
.806
40.
183
11.8
534
0.35
810
.343
80.
679
11.3
079
1.16
610
.141
60.
161
11.1
552
0.32
49.
6721
0.65
910
.633
21.
145
9.46
990.
162
10.4
832
0.28
88.
9867
0.70
29.
9676
1.14
58.
7844
0.14
09.
8148
0.21
98.
2833
0.70
49.
2898
1.16
18.
0775
0.16
99.
1332
0.66
98.
5935
0.16
18.
3450
0.60
27.
8781
0.15
87.
7911
Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998 597
-
Tab
le1.
(Con
tin
ued
)
P/M
Pa
F/m
oL-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF/
mol
L-
1P
/MP
aF
/moL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
P/M
Pa
F/m
olL
-1
x 1)
0.90
61T
)25
7.51
KT
)27
2.93
KT
)30
2.40
KT
)33
2.99
KT
)36
3.27
KT
)38
3.59
KT
)40
4.03
KT
)42
4.40
KT
)44
2.56
K18
.914
30.2
487
19.0
5929
.606
328
.993
28.5
177
38.4
5927
.561
338
.268
26.2
995
39.0
9425
.551
440
.274
24.8
076
38.8
4424
.112
219
.764
22.9
994
17.4
9330
.201
617
.594
29.5
571
27.5
1628
.468
136
.978
27.5
053
36.8
4126
.249
137
.625
25.5
058
38.7
8824
.762
237
.376
24.0
690
18.3
0722
.959
216
.060
30.1
587
16.1
2329
.508
926
.062
28.4
153
35.5
3727
.452
635
.359
26.2
044
36.1
1725
.458
237
.311
24.7
193
35.8
8224
.025
016
.801
22.9
246
14.6
4830
.119
414
.635
29.4
520
24.5
9828
.358
434
.076
27.3
981
33.8
8626
.152
634
.657
25.4
145
35.7
9024
.673
634
.414
23.9
801
15.3
0722
.885
113
.225
30.0
784
13.1
5529
.404
023
.165
28.3
060
32.6
5127
.344
332
.385
26.1
079
33.2
4525
.379
234
.276
24.6
294
32.9
3923
.936
913
.776
22.8
447
11.7
8830
.025
311
.678
29.3
572
21.6
9528
.248
531
.196
27.2
954
30.9
4726
.061
131
.734
25.3
401
32.7
8824
.582
631
.417
23.8
973
12.3
0222
.808
910
.326
29.9
779
10.2
4229
.298
620
.239
28.1
926
29.7
2727
.240
829
.480
26.0
177
30.2
6925
.295
031
3.19
24.5
374
29.8
8623
.855
810
.781
22.7
747
8.85
229
.934
28.
747
29.2
417
18.7
7428
.138
128
.248
27.1
897
27.9
8125
.972
428
.798
25.2
473
29.8
5124
.494
428
.384
23.8
192
9.32
222
.737
07.
416
29.8
912
7.26
929
.187
517
.289
28.0
842
26.7
7927
.136
426
.501
25.9
228
27.2
9725
.200
928
.350
24.4
538
26.9
2323
.780
07.
781
22.6
980
6.03
229
.852
35.
817
29.1
337
15.8
1728
.038
225
.321
27.0
908
25.0
2425
.874
925
.863
25.1
573
26.8
1624
.416
225
.466
23.7
400
6.36
022
.662
14.
587
29.8
090
4.39
029
.087
414
.353
27.9
871
23.8
3027
.040
923
.562
25.8
275
24.4
0125
.112
825
.341
24.3
708
23.9
7123
.703
95.
001
22.6
290
3.22
429
.762
52.
747
28.9
781
12.8
8227
.935
122
.394
26.9
868
22.0
7825
.788
622
.942
25.0
730
23.8
4224
.326
722
.437
23.6
635
3.66
622
.598
511
.416
27.8
850
20.9
5826
.936
620
.620
25.7
472
21.4
6525
.035
322
.376
24.2
870
21.0
0923
.624
82.
411
22.5
662
9.96
027
.839
719
.456
26.8
974
19.1
1625
.709
720
.062
24.9
914
20.8
7224
.243
919
.559
23.5
865
2.28
120
.227
58.
560
27.7
918
18.0
3026
.853
217
.617
25.6
711
18.6
5524
.944
319
.364
24.2
018
18.1
3623
.548
82.
222
17.2
814
7.25
127
.748
916
.552
26.8
133
16.1
4125
.621
317
.210
24.9
003
17.8
9924
.160
916
.665
23.5
096
2.20
215
.324
55.
782
27.7
098
15.1
0026
.766
914
.639
25.5
772
15.8
6324
.858
416
.404
24.1
186
15.1
9923
.469
92.
209
13.8
082
4.41
227
.664
313
.659
26.7
167
13.1
8125
.534
014
.475
24.8
157
14.9
4924
.075
313
.715
23.4
328
2.17
512
.591
53.
066
27.6
200
12.2
0226
.672
111
.692
25.4
882
13.0
3924
.774
113
.491
24.0
321
12.2
1323
.398
92.
164
11.6
220
1.68
927
.575
910
.797
26.6
307
10.2
1525
.446
211
.683
24.7
284
12.0
1223
.992
110
.736
23.3
582
2.17
710
.816
51.
149
27.5
239
9.34
326
.591
08.
758
25.3
992
10.6
1624
.687
710
.594
23.9
512
9.28
423
.319
52.
159
10.1
322
7.86
626
.541
87.
404
25.3
558
9.28
424
.642
69.
188
23.9
116
7.87
223
.281
72.
185
9.52
196.
412
26.4
972
6.04
525
.315
57.
948
24.6
057
7.81
523
.873
76.
410
23.2
436
2.14
78.
9521
5.06
426
.456
84.
699
25.2
744
6.66
624
.564
96.
364
23.8
374
5.01
823
.203
52.
153
8.40
533.
618
26.4
181
3.34
025
.236
25.
284
24.5
226
4.96
023
.806
43.
615
23.1
644
2.15
67.
8570
2.23
626
.381
22.
035
25.1
996
3.99
924
.476
83.
685
23.7
673
2.28
323
.127
42.
131
7.29
371.
162
26.3
354
1.15
125
.135
42.
757
24.4
393
2.32
023
.730
51.
284
18.5
580
2.13
36.
7156
0.13
719
.943
31.
424
24.0
876
1.17
723
.475
41.
271
16.0
603
0.13
117
.110
41.
140
23.9
545
0.92
420
.810
71.
264
14.0
741
0.12
514
.925
30.
493
21.3
949
0.91
517
.825
21.
259
12.6
164
0.12
013
.463
20.
490
18.5
063
0.91
115
.772
11.
256
11.5
497
0.10
212
.310
70.
485
16.0
653
0.88
214
.146
31.
260
10.6
796
0.11
711
.383
20.
491
14.3
747
0.91
012
.870
61.
254
10.0
002
0.10
810
.615
50.
468
13.0
483
0.88
411
.851
21.
248
9.35
630.
120
9.95
270.
445
11.9
854
0.86
811
.012
11.
246
8.79
820.
134
9.35
130.
451
11.1
194
0.86
310
.300
91.
228
8.25
450.
120
8.79
020.
450
10.3
901
0.85
49.
6773
1.19
57.
7078
0.10
98.
2387
0.42
39.
7495
0.86
69.
1032
1.22
97.
1414
0.10
87.
6822
0.45
09.
1692
0.86
38.
5547
1.22
36.
5635
0.10
87.
1080
0.43
08.
6170
0.84
57.
9663
0.10
36.
5221
0.41
98.
0683
0.83
97.
3512
0.45
37.
5117
0.83
36.
7266
0.43
66.
9399
0.42
46.
3566
598 Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998
-
tion defined by
are given in Table 5 where NP and Ny are respectively thenumbers of determinations of bubble-point pressures andof vapor-phase compositions.
The vapor-liquid equilibrium of methanol + water hasbeen measured by Griswold and Wong (1952) between373.15 K and 523.15 K, by Schroder (1958) at 413.15 K,and by Hirata and Suda (1967) and Hirata et al. (1975)
at pressures of 0.3 MPa and 0.5 MPa. The results obtainedfrom these authors and our data are summarized in Table6. The agreement is satisfactory. Moreover, we canremark in Figure 4 that our own measurements at 424.15K agree with those of Griswold and Wong (1952) at 423.15K, the only reference temperature.
Conclusion
We have described a high-pressure apparatus designedto obtain pressure-density-temperature data of a pure-component or a mixture over the temperature range 210K-470 K and at pressures up to 70 MPa. The densities of
Figure 2. Schematic diagram of the measurement cell: (1) saphirwindows; (2) stainless steel valve; (3) fluid introduction; (4)internal iron kernel for the stirrer; (5) stirrer support; (6) stirrer;(7) external iron kernel for the stirrer; (8) copper cylinder; (9)copper column; (10) bellow; (11) chamber; (12) copper rod; (13)thermocouple; (14) column connecting the support of the externalstirrer with the micrometric table; (15) low position of the stirrer;(16) cooper mass for transferring the heating or cooling fluid tothe bottom of the bellow; (17) cooling circuit; (18) entrance tube ofthe compression fluid; (19) cooling platform; (20) entrance of liquidnitrogen.
P/P(%) )100
NPi)1
NP jPexp,i - Pcal,iPexp,i j (7)y )
1
Nyi)1
Ny
jyexp,i - ycal,ij (8)
Figure 3. Determination of bubble pressure of methanol (1) +water (2) at 363.15 K for x1 ) 0.4980: [, data in single-phaseregion (liquid); 9, data in two-phase region; 2, data in two-phaseregion not taken into account in linear regression.
Table 2. Bubble Pressures for the Methanol (1) + Water(2) System at Five Different Temperatures
P/MPa
x1 363.15 K 383.15 K 403.15 K 424.15 K 442.15 K
0.1061 0.117 0.227 0.403 0.665 1.1570.2872 0.153 0.293 0.567 0.937 1.4770.4980 0.181 0.369 0.647 1.073 1.7040.6876 0.219 0.401 0.715 1.218 1.9060.9061 0.238 0.458 0.844 1.296 2.093
Table 3. Comparison of Experimental and CalculatedLiquid-Phase Density Data at Selected Temperaturesand Pressures
T/Kpressure
range (MPa)no. ofdata F/F (%) r(F)
332.55 13.751-1.150 44 2.63 -0.30363.17 13.052-1.062 46 2.62 -1.17383.57 13.039-0.995 46 2.89 -1.75403.52 12.896-0.942 45 2.97 -1.96424.05 12.937-2.126 40 2.85 -1.81443.50 12.763-2.411 37 3.18 -1.76
Table 4. Pure Component Parameters Used in ThisStudy
compd Tc/K Pc/MPa Tb/K b/cm3mol-1 m1 m2
methanol 512.58 8.094 337.70 23.995 1.080 64 -0.170 98water 647.37 22.120 373.15 11.089 1.358 60 0.165 64
Table 5. Vapor-Liquid Equilibrium Results forMethanol + Water
type ref
temprange
(K)
pressurerange(MPa) NP P/P (%) Ny y
isothermal 1 to 13 243-474 0.00005-3.950 449 1.86 262 0.018
isobaric 14 to 39 307-421 0.026-0.507 422 2.13 387 0.011
global 871 1.99 649 0.014
Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998 599
-
the methanol + water have been measured in the single-phase and two-phase region. The VLE pressure-composi-tion data obtained from densities are in good agreementwith literature values that have been fitted to the excessfunction-equation of state model by adjusting an interactionparameter.
Literature CitedBenson, G. C.; Kiyohara, O. Thermodynamics of Aqueous Mixtures of
Non-Electrolytes. 1. Excess Volumes of Water-N-Alcohol Mixturesat Several Temperatures. J. Solution Chem. 1980, 9, 791-804.
Easteal, A. J.; Woolf, L. A. (P, Vm, T, X) Measurements for ((1-x)H2O+ xCH3OH) in the Range 278 K to 323 K and 0.1 to 280 MPA. 2.Thermodynamic Excess Properties. J. Chem. Thermodyn. 1985, 17,69-82.
Goodwin, R. D. Methanol thermodynamic properties from 176 to 673K at pressures to 700 bar. J. Phys. Chem. Ref. Data 1987, 16, 799-892.
Goodwin, R. D. Toluene thermophysical properties from 178 to 800 Kat pressures to 1000 bar. J. Phys. Chem. Ref. Data 1989, 18, 1565-1636.
Griswold, J.; Wong, S. Y. Phase-Equilibria of the Acetone-Methanol-Water System from 100 C into the Critical Region. Chem. Eng.Prog., Symp. Ser. 1952, 48, 18-25.
Hirata, M.; Suda, S. Vapor Pressure of Methanol in High-PressureRegions. Kagaku Kogaku 1967, 31, 339-341.
Hirata, M.; Ohe, S.; Nagahama, K. Computer aided data of VLE;Elsevier: Amsterdam, 1975.
Hocq, H. Ph.D. Thesis, University Aix-Marseille II, France, 1994; pp1-289.
Hocq, H.; Bur, Y.; Berro, C. Densities of liquid water, toluene, andmethanol at 240 to 450 K and up to 70 MPa and of gaseous methanolat 420 to 450 K and up to 2 MPa. ELDATA: Int. Electron. J. Phys.-Chem. Data 1995, 1, 79-86.
McGlashan, M. L.; Williamson, A. G. Isothermal Liquid-VaporEquilibria for System Methanol-Water. J. Chem. Eng. Data 1976,21, 196-199.
Patel, N. C.; Sandler, S. I. Excess Volumes of the Water/Methanol,n-Heptane/Ethyl Acetate, n-Heptane/n-Butyraldehyde, and n-Hep-tane/Isobutyraldehyde Systems. J. Chem. Eng. Data 1985, 30, 218-222.
Peneloux, A.; Abdoul, W.; Rauzy, E. Excess functions and equationsof state. Fluid Phase Equilib. 1989, 47, 115-132.
Schroder, W. Measuring vapor-liquid equilibria at elevated pressure.Chem.-Ing.-Tech. 1958, 30, 523-525.
Xiao, C.; Bianchi, H.; Tremaine, P. R. Excess molar volumes anddensities of methanol + water at temperatures between 323 K and573 K and pressures of 7.0 MPa and 13.5 MPa. J. Chem. Thermodyn.1997, 29, 261-286.
Received for review December 13, 1997. Accepted April 6, 1998.The authors acknowledge with gratitude the society TOTAL fortheir financial support through FSH and ARTEP.
JE970297P
Figure 4. Vapor-liquid equilibria of the methanol-water binarysystem at 424.15 K. Calculated curve: full line. Data: *, our work;0, Griswold and Wong at 423.15 K.
Table 6. Relative Mean Deviations in the Bubble-PointPressure for Our Data and Those Reported in theLiterature
T/K P/MPa NP P/P (%) ref
363.15 5 1.76 our work383.15 5 1.33 our work403.15 5 2.79 our work424.15 5 2.67 our work442.15 5 1.10 our work373.15 18 1.54 Griswold and Wong423.15 16 0.81 Griswold and Wong473.15 17 3.82 Griswold and Wong413.15 6 1.29 Schroeder
0.304 10 2.96 Hirata and Suda0.507 11 2.14 Hirata. and Suda0.304 26 1.78 Hirata et al.0.507 26 2.21 Hirata et al.
600 Journal of Chemical and Engineering Data, Vol. 43, No. 4, 1998