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Speeds of sound in {(1 − x)CH 4 + xN 2} with x = (0.10001, 0.19999, and 0.5422) at temperatures between 170 K and 400 K and pressures up to 30 MPa
The speed of sound in {(1 − x)CH 4 + xN 2} has been measured with a spherical acoustic resonator. Two mixtures with x = (0.10001 and 0.19999) were studied along isotherms at temperatures between 220 K and 400 K with pressures up to 20 MPa; a few additional measurements at p = (25 and 30) MPa are als...
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Published in: | The Journal of chemical thermodynamics 2006-07, Vol.38 (7), p.929-937 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | The speed of sound in {(1
−
x)CH
4
+
xN
2} has been measured with a spherical acoustic resonator. Two mixtures with
x
=
(0.10001 and 0.19999) were studied along isotherms at temperatures between 220
K and 400
K with pressures up to 20
MPa; a few additional measurements at
p
=
(25 and 30)
MPa are also reported. A third mixture with
x
=
0.5422 was studied along pseudo-isochores at amount-of-substance densities between 0.2
mol
·
dm
−3 and 5
mol
·
dm
−3. Corrections for molecular vibrational relaxation are discussed in detail and relaxation times are reported. The overall uncertainty of the measured speeds of sound is estimated to be not worse than ±0.02%, except for those measurements in the mixture with
x
=
0.5422 that lie along the pseduo-isochore at the highest amount-of-substance density. The results have been compared with the predictions of several equations of state used for natural gas systems. |
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ISSN: | 0021-9614 1096-3626 |
DOI: | 10.1016/j.jct.2005.10.006 |