๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Speed of sound in carbon dioxide at temperatures between (220 and 450) K and pressures up to 14 MPa

โœ Scribed by A.F. Estrada-Alexanders; J.P.M. Trusler


Publisher
Elsevier Science
Year
1998
Tongue
English
Weight
205 KB
Volume
30
Category
Article
ISSN
0021-9614

No coin nor oath required. For personal study only.

โœฆ Synopsis


The speed of sound u in carbon dioxide has been measured along seven isotherms at ลฝ . temperatures between 220 and 450 K by means of a spherical resonator. At supercritical temperatures, the greatest pressure on each isotherm was chosen to correspond to approximately one-half of the critical density while, at subcritical temperatures, the greatest pressure on each isotherm was limited to that at which the density was about 80 per cent of the saturated vapour density. Vibrational relaxation, which is severe in pure carbon dioxide at frequencies of the order 10 kHz when the pressure is below p s 1 MPa, necessitates significant corrections for dispersion and leads to greatly enhanced sound absorption, which limits the precision of the measurements somewhat. Nevertheless, the results have an overall estimated . y4 uncertainty which varies from 3 10 u at the lowest temperature and pressure studied, to . y5 better than 5 10 u at p G 1 MPa. The results have been analysed to obtain both second and third acoustic virial coefficients, and ordinary second virial coefficients.


๐Ÿ“œ SIMILAR VOLUMES


The speed of sound in gaseous argon at t
โœ A.F. Estrada-Alexanders; J.P.M. Trusler ๐Ÿ“‚ Article ๐Ÿ“… 1995 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 485 KB

The speed of sound u in gaseous argon has been measured along 21 isotherms at temperatures T between 110 K and 450 K. At Te150 K, the greatest pressure on each isotherm was the lesser of 19 MPa and the pressure at which the estimated density was half its critical value. Below T=150 K, the greatest p

The speed of sound and derived thermodyn
โœ A.F. Estrada-Alexanders; J.P.M. Trusler ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 286 KB

The speed of sound u in gaseous ethane of mole-fraction purity 0.9999 has been measured along 17 isotherms at temperatures between 220 K and 450 K. At temperatures of 300 K and above, the greatest pressure on each isotherm was chosen to correspond to that at approximately one half of the critical de

The speed of sound in gaseous propane at
โœ J.P.M. Trusler; M.P. Zarari ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 332 KB

The speed of sound in gaseous propane has been measured along seven isotherms in the temperature range 225 K to 375 K at pressures up to the lower of 0.85 MPa and 80 per cent of the vapour pressure. The results have a precision of 0.001 per cent or better and an overall uncertainty, including an all

The speed of sound in nitrogen at temper
โœ M.F Costa Gomes; J.P.M Trusler ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 152 KB

The speed of sound has been measured in nitrogen on four isotherms at TrK s 250, 275, 300, and 350, and at pressures between 0.1 MPa and 30 MPa. The measurements were made using a spherical resonator operating at frequencies between 5 kHz and 26 kHz where the speed of sound in nitrogen differs signi

The speed of sound in two methane-rich g
โœ M.F. Costa Gomes; J.P.M. Trusler ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 132 KB

The speed of sound has been measured in two methane-rich gas mixtures having nominal ลฝ . ลฝ compositions of 0.85CH q 0.15C H and 0.80CH q 0.10N q 0.05C H q 0.03C H q 4 2 6 4 2 2 6 3 8 . 0.02CO . The measurements were made with a spherical acoustic resonator on four 2 isotherms at TrK s 250, 275, 300

Speed of sound in (0.4C2H6 + 
โœ A.F. Estrada-Alexanders; J.P.M. Trusler ๐Ÿ“‚ Article ๐Ÿ“… 1999 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 126 KB

The speed of sound u has been measured in {(1x 2 )C 2 H 6 + x 2 CO 2 }, with x 2 โ‰ˆ 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