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Physical & Chemical properties

Vapour pressure

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Reference
Endpoint:
vapour pressure
Type of information:
experimental study
Adequacy of study:
key study
Reliability:
1 (reliable without restriction)
Rationale for reliability incl. deficiencies:
guideline study
Qualifier:
according to guideline
Guideline:
OECD Guideline 104 (Vapour Pressure Curve)
Deviations:
not specified
Qualifier:
according to guideline
Guideline:
EU Method A.4 (Vapour Pressure)
Deviations:
not specified
GLP compliance:
no
Type of method:
other: Combination of "effusion method: by loss of weight or by trapping vaporisate" and "static method"
Key result
Temp.:
20 °C
Vapour pressure:
0 Pa
Remarks on result:
other: calculated from experimental values
Temp.:
25 °C
Vapour pressure:
0 Pa
Remarks on result:
other: calculated from experimental values
Temp.:
49.95 °C
Vapour pressure:
0.01 Pa
Remarks on result:
other: experimental result (Knudsen effusion method, average of two measurements)
Temp.:
50 °C
Vapour pressure:
0.01 Pa
Remarks on result:
other: calculated from experimental values
Temp.:
55 °C
Vapour pressure:
0.02 Pa
Remarks on result:
other: calculated from experimental values
Temp.:
59.95 °C
Vapour pressure:
0.045 Pa
Remarks on result:
other: experimental result (Knudsen effusion method, average of two measurements)
Temp.:
69.95 °C
Vapour pressure:
0.127 Pa
Remarks on result:
other: experimental result (Knudsen effusion method, average of two measurements)
Temp.:
90 °C
Vapour pressure:
1.3 Pa
Remarks on result:
other: experimental result (static method, average of three measurements)
Temp.:
110 °C
Vapour pressure:
8.54 Pa
Remarks on result:
other: experimental result (static method, average of three measurements)
Temp.:
129.2 °C
Vapour pressure:
46.37 Pa
Remarks on result:
other: experimental result (static method, average of three measurements)

Results obtained in the measurement of the vapor pressures of dibutyl hydrogen phosphate using the Knudsen effusion method.

 

T / °C = 49.95    t = 19h36m46s

Cell

m / mg

p / Pa

I

1.87

0.0100

IV

1.76

0.0093

  

T / °C = 59.95    t = 07h27m42s

Cell

m / mg

p / Pa

I

3.40

0.0485

IV

2.97

0.0418

  

T / °C = 69.95    t = 03h52m58s

Cell

m / mg

p / Pa

I

4.79

0.1333

IV

4.40

0.1207

  

T / °C = 79.90    t = 02h49m38s

Cell

m / mg

p / Pa

I

10.35

0.4012

IV

8.97

0.3428

  

 

Results obtained in the measurement of the vapor pressures of dibutyl hydrogen phosphate using the static method.

 

T / K

T / °C

p / Pa

p / mbar

90.00

363.15

1.30

0.013

99.40

372.55

3.18

0.0318

110.00

383.15

8.54

0.0854

119.30

392.45

18.47

0.1847

129.20

402.35

46.37

0.4637

 

 

Recommended vapor pressures for dibutyl hydrogen phosphate up to 240 °C, calculated from the application of the equation of Clarke and Glew to the results obtained in this work.

 

T / °C

T / K

p / Pa

p / mbar

-20

253.15

4.75E-08

4.75E-010

-15

258.15

1.45E-07

1.45E-09

-10

263.15

4.22E-07

4.22E-09

-5

268.15

1.18E-06

1.18E-08

0

273.15

3.16E-06

3.16E-08

5

278.15

8.17E-06

8.17E-08

10

283.15

2.04E-05

2.04E-07

15

288.15

4.91E-05

4.91E-07

20

293.15

1.15E-04

1.15E-06

25

298.15

2.59E-04

2.59E-06

30

303.15

5.70E-04

5.70E-06

35

308.15

1.22E-03

1.22E-05

40

313.15

2.54E-03

2.54E-05

45

318.15

5.17E-03

5.17E-05

50

323.15

1.03E-02

1.03E-04

55

328.15

1.99E-02

1.99E-04

60

333.15

3.78E-02

3.78E-04

65

338.15

7.04E-02

7.04E-04

70

343.15

1.28E-01

1.28E-03

75

348.15

2.30E-01

2.30E-03

80

353.15

4.05E-01

4.05E-03

85

358.15

7.00E-01

7.00E-03

90

363.15

1.19E+00

1.19E-02

95

368.15

1.99E+00

1.99E-02

100

373.15

3.28E+00

3.28E-02

105

378.15

5.34E+00

5.34E-02

110

383.15

8.55E+00

8.55E-02

115

388.15

1.35E+01

1.35E-01

120

393.15

2.11E+01

2.11E-01

125

398.15

3.26E+01

3.26E-01

130

403.15

4.96E+01

4.96E-01

135

408.15

7.48E+01

7.48E-01

140

413.15

1.11E+02

1.11E+00

145

418.15

1.64E+02

1.64E+00

150

423.15

2.40E+02

2.40E+00

155

428.15

3.46E+02

3.46E+00

160

433.15

4.96E+02

4.96E+00

165

438.15

7.04E+02

7.04E+00

170

443.15

9.89E+02

9.89E+00

175

448.15

1.38E+03

1.38E+01

180

453.15

1.91E+03

1.91E+01

185

458.15

2.62E+03

2.62E+01

190

463.15

3.56E+03

3.56E+01

195

468.15

4.81E+03

4.81E+01

200

473.15

6.46E+03

6.46E+01

205

478.15

8.60E+03

8.60E+01

210

483.15

1.14E+04

1.14E+02

215

488.15

1.50E+04

1.50E+02

220

493.15

1.96E+04

1.96E+02

225

498.15

2.54E+04

2.54E+02

230

503.15

3.28E+04

3.28E+02

235

508.15

4.21E+04

4.21E+02

240

513.15

5.37E+04

5.37E+02

 

Conclusions:
The vapor pressure of dibutyl hydrogen phosphate is 0.000115 Pa at 20 °C.
Executive summary:

The vapor pressure of dibutyl phosphate was measured using the Knudsen effusion method (mass-loss technique) and a static method suitable for very low vapor pressures, according to the guidelines OECD 104 / EU A.4.

The quality of both apparatus was previously verified with the measurement of well-known reference compounds. Experiments were performed at temperatures between 50 °C and 80 °C using the Knudsen effusion method, and between 80 °C and 130 °C using the static method.

Results were modeled with a thermodynamic equation, establishing the relation between the vapor pressure of the compound and temperature and allowing the knowledge of the vapor pressure at different temperatures.

Description of key information

The vapor pressure of dibutyl hydrogen phosphate is 0.000115 Pa at 20 °C.

Key value for chemical safety assessment

Vapour pressure:
0 Pa
at the temperature of:
20 °C

Additional information

The vapor pressure of dibutyl phosphate was measured using the Knudsen effusion method (mass-loss technique) and a static method suitable for very low vapor pressures, according to the guidelines OECD 104 / EU A.4.

Results were modeled with a thermodynamic equation, establishing the relation between the vapor pressure of the compound and temperature and allowing the knowledge of the vapor pressure at different temperatures.

The vapor pressure of dibutyl hydrogen phosphate can be calculated using the following truncated equation of Clarke and Glew.

ln(p) = exp({- (ΔG / θ) + ΔH * [(1 / θ) + (1 / T)] + ΔC * [(θ / T) - 1 + ln(T / θ)]} / R)

Where p is the vapour pressure in Pa, T is the temperature in Kelvin, ΔG is the Gibbs energy of vaporization at the reference temperature θ [-389.82 J/mol], ΔH is the enthalpy of vaporization at the reference temperature θ [114715 J/mol], ΔC is the difference between the heat capacity of the gas and the heat capacity of the liquid at the reference temperature θ [-60 J/(mol K)], θ is the reference temperature [362.72 K] and R is the gas constant [8.3144621 J/(mol K)].