Measurements of ( p, ρ, T ) for {x NH 3 + (1 -x)H 2 O} at x = (1.0000, 0.8374, 0.6005, and 0.2973) and at specified temperatures and pressures in the compressed liquid phase were carried out with a metal-bellows variable volumometer between T = 310 K and T = 400 K at pressures up to 17 MPa. The resu
Thermodynamic properties of {xCH3OH  + (1−x)H2O} withx =  (1.0000 and 0.4993) in the temperature range from 320 K to 420 K at pressures up to 200 MPa
✍ Scribed by O. Osada; M. Sato; M. Uematsu
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 175 KB
- Volume
- 31
- Category
- Article
- ISSN
- 0021-9614
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✦ Synopsis
Measurements of ( p, ρ, T ) for {xCH 3 OH + (1x)H 2 O} with x = (1.0000 and 0.4993) at specified temperatures and pressures in the compressed liquid phase were carried out with a metal-bellows variable volumometer along six isotherms between T = 320 K and T = 420 K at pressures from the bubble point pressure to p = 200 MPa. The results cover the high-density region from ρ = 884 kg•m -3 to ρ = 651 kg•m -3 for x = 1.0000, and from ρ = 948 kg•m -3 to ρ = 755 kg•m -3 for x = 0.4993. The experimental uncertainties in temperature T , pressure p, density ρ, and mole fraction x were estimated to be less than ±3 mK, ±1.0•10 -3 • p, ±1.0•10 -3 •ρ, and ±1.0•10 -3 • x, respectively. Measurements of vapour pressure, bubble point pressure, and saturated liquid density at temperatures from 320 K to 420 K are also reported. On the basis of the present results, the excess molar volumes for (0.4993CH 3 OH + 0.5007H 2 O) were calculated and are tabulated as a function of temperature and pressure.
📜 SIMILAR VOLUMES
The speed of sound u has been measured in {(1x 2 )C 2 H 6 + x 2 CO 2 }, with x 2 ≈ 0.6, along seven isotherms at temperatures between T = 220 K and T = 450 K by means of a spherical resonator. The greatest pressure on each isotherm was approximately p = 1.2 MPa except at T = 220 K where, to avoid co
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