Evaluator
Peter G.T. Fogg School of Applied Chemistry, University of North LondonEvaluation
It is often helpful to compare experimental values of mole fraction solubility x1, of a gas at a particular temperature with reference values from the Raoult's law equation
where po is the vapour pressure of liquefied gas at the temperature in question. The variation with temperature of p1/po provides a reference line for comparison of solubility. The critical temperature of ethene is 282.4 K but it is convenient to extrapolate the vapour pressure of ethene to temperatures above the critical temperature to calculate a reference line and hence facilitate qualitative comparison of experimental solubility. Mole fraction solubility in most solvents containing oxygen fall below the reference line and are low compared with solubility in straight chain hydrocarbons.
2-Propanone; C3H6O; [67-64-1]
Solubility in 2-propanone has been measured by Horiuti1, Hannaert et al.2, Leites and Ivanovskii3, and by McDaniel4. McDaniel's values for a partial pressure of 101.3 kPa fall appreciably below those given by Horiuti and can be disregarded because other measurements by McDaniel have been found to be significantly lower than measurements carried out more recently. Solubility values calculated from equations given by Hannaert for 283.15 K and 293.15 K are, respectively, about 18% and 14% above values given by Horiuti. Horiuti's data for the temperature range of 273.15 to 313.15 K is likely to be the more reliable. A measurement carried out by this author on other systems is often in close agreement with more recent precision measurements. Horiuti's data can be fitted to the equation:
where x1 is the mole fraction solubility at p1 = 101.3 kPa standard deviation in values of x1 = 2.0 × 10-5 temperature range 273 K to 313 K This equation may be accepted on a tentative basis.
The following equation is based upon Horiuti's measurements from 273.15 K to 313.15 K, on Flannaert's measurements from 243.15 K to 293.15 K and on the single value at 243.15 K given by Leites and Ivanovskii.
ln x1 = -8.5070 + 1195.3/(T/K)
standard deviation in values of x1 = 8.5 × 10-4 temperature range 243 K to 313 K.
This equation is recommended on a tentative basis for temperatures below 273 K.
Methyl acetate; C3H6O2 [79-20-9]
Horiuti1 also measured solubility in methyl acetate. Mole fraction solubility at a partial pressure of 101.3 kPa fit the equation:
ln x1 = 3.2620 + 569.63/(T/K) - 1.6935 ln(T/K)
standard deviation in values of x1 = 3.4 × 10-5 temperature range 273 K to 313 K.
Horiuti's data for methyl acetate is classified as tentative.
Cyclopentanone; C5H80; [120-92-3]
Cyclohexanone; C6H100; [108-94-1]
2-Methylcyclohexanone; C7H120; [583-60-8]
2, 6-Dimethylcyclohexanone; C8H140; [2816-57-1]
Gallardo and co-workers have measured solubility in cyclic ketones5-9 at a partial pressure of ethene of 101.3 kPa in the temperature 273.15 K to 303.15 K. Mole fraction solubility at the same temperature in these solvents are in the order 2,6-dimethylcyclohexanone > 2-methyl-cyclohexanone > cycloheptanone > cyclohexanone > cyclopentanone. Sets of measurements are consistent with each other (see Fig.1).) and all fall below the reference line based on Raoult's law in this temperature range.
Solubility at a partial pressure of gas of 101.3 kPa may be fitted to the following equations derived by the evaluator. These give slightly better fit than equations given by the authors.
2,6-dimethylcyclohexanone
ln x1 = - 8.5574 + 1294.9/(T/K)
standard deviation in values of x1 = 3.4 × 10-5
2-methylcyclohexanone
ln x1 = 41.885 - 980.94/(T/K) - 7.5339 ln(T/K)
standard deviation in values of x1 = 5.9 × 10-5
cycloheptanone
ln x1 = -22.106 + 1764.3/(T/K) + 2.0544 ln(T/K)
standard deviation in values of x1 = 2.4 × 10-5
cyclohexanone
ln x1 = 35.451 - 773.66/(T/K) - 6.5627 ln(T/K)
standard deviation in values of x1 = 2.9 × 10-5
cyclopentanone
In x1 = 25.679 - 337.58/(T/K) - 5.1162 ln(T/K)
standard deviation in values of x1 = 1.4 × 10-5
These equations may be accepted on a tentative basis for the temperature range 273.15 K to 303.15 K.
4-Methyl-1,3-dioxolan-2-one (propylene carbonate); C4H6O3 [108-32-71]
Henry's constants for dissolution of ethene in 4-methyl-1,3-dioxolan-2-one was measured by a chromatographic method at 298.2 K to 343.2 K by Lenoir et al.10. Mole fraction solubility at 298.2 K and a partial pressure of 101.3 kPa, calculated on the assumption of a linear variation of mole fraction solubility with partial pressure, is 0.00521 compared with 0.00421 from measurements by Briickl and Kim11. Solubility reported by Lenoir et al. for some of the other systems which they have studied are high compared with measurements by other groups. This is probably due to limitations of the chromatographic method. Further measurements on this system are required.
1,2-Epoxyhexane; C6H12O; [592-90-5]
Mole fraction solubility measured by Gibanel et al.12 at a partial pressure of 101.3 kPa in 1,2-epoxyhexane fall in between solubility in 2-methylcyclohexanone and 2,6-dimethylcyclohexanone. The data may be fitted to the equation
ln x1 = -50.928 + 3025.0/(T/K) + 6.4117 ln(T/K)
standard deviation in values of x1 = 2.9 × 10-5 temp. range 273 K to 303 K
This equation may be accepted on a tentative basis.
1,4-Dioxane; C4H8O2 [123-91-1]
Solubility in the cyclic diether, 1,4-dioxane is low compared with that in cyclic ketones. Solubility at a partial pressure of ethene of 101.3 kPa reported by Gallardo et al.13 for the temperature range 285.15 K to
303.15 K fit the equation
ln x1 = -1.2404 + 763.88/(T/K) - 1.0499 ln(T/K)
standard deviation in values of x1 = 1.7 × 10-5
This equation fits the data better than the one given by the authors and may be accepted on a tentative basis.
1, 1'-[Methylenebis(oxy)]-bisethane; C5H12O2
The mole fraction solubility reported by Lizano et al.14 at a partial pressure of 101.3 kPa in the acetal, 1,1'-[methylenebis(oxy)]-bisethane, is higher than that in the cyclic ketones (see Fig. 1). Values lie above the reference line based upon the Raoult's law equation. The data may be fitted to the equation
ln x1 = -17.138 + 1927.7/(T/K) + 1.1882 ln(T/K)
standard deviation in values of = 2.6 × 10-5 temp. range 263 K to 303 K
This equation may be accepted on a tentative basis.
Figure
Sources:
2
Hannaert, H.; Haccuria, M.; Mathieu, M. P.; Ind. Chim. Belge 1967, 32, 156-164.
3
Leites, I. L.; Ivanovskii, F. P.; Khim. Prom. 1962, 9, 653-657.
4
McDaniel, A. S.; J. Phys. Chem. 1911, 15, 587-610.
5
Gallardo, M. A.; Lopez, M. C.; Urieta, J. S.; Gutierrez Losa, C.; Fluid Phase Equilib. 1989, 50, 223-233.
6
Gallardo, M. A.; Melendo, J. M.; Urieta, J. S.; Gutierrez Losa, C.; Can. J. Chem. 1987, 65, 2198-2202.
7
Gallardo, M. A.; Carmen Lopez, M.; Urieta, J. S.; Gutierrez Losa, C.; Can. J. Chem. 1989, 67, 809-811.
8
Gallardo, M. A.; Lopez, M. C.; Urieta, J. S.; Gutierrez-Losa, C.; Can. J. Chem. 1990, 68, 435-439.
9
Gallardo, M. A.; Lopez, M. C.; Urieta, J. S.; Gutierrez-Losa, C.; Fluid Phase Equilib. 1990, 58, 159-172.
10
Lenoir, J-Y.; Renault, P.; Renon, H.; J. Chem. Eng. Data 1971, 16, 340-2.
11
Brückl, N.; Kim, J. I.; Z. Phys. Chem. 1981, 126, 133-150.
12
Gibanel, F.; Lopez, M. C.; Gallardo, M. A.; Urieta, J. S.; Gutierrez Losa, C.; Fluid Phase Equilib. 1988, 42, 261-268.
13
Gallardo, M. A.; Urieta, J. S.; Gutierrez Losa, C., J. Chim. Phys. 1983, 80, 621.
14
Lizano, L. P.; López, M. C.; Royo, F. M.; Urieta, J. S.; J. Solution Chem. 1990, 19, 721-728.
1
Horiuti, J.; Sci. Pap. Inst. Phys. Chem. Res. (Jpn) 1931/32, 17, 125 - 256.