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Speeds of sound, densities, refractive indices, and isentropic compressibilities of {x1C6H6 + x2c-C6H12 + (1 - x1 - x2)C6H5Cl} at the temperature 298.15 K

✍ Scribed by M. Iglesias; B. Orge; J. Tojo

Publisher
Elsevier Science
Year
1994
Tongue
English
Weight
159 KB
Volume
26
Category
Article
ISSN
0021-9614

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✦ Synopsis

Speeds of sound, densities, refractive indices, and isentropic compressibilities, at the temperature (298.15 \mathrm{~K}) of (\left{x_{1} \mathrm{C}{6} \mathrm{H}{6}+x_{2} \mathrm{c}-\mathrm{C}{6} \mathrm{H}{12}+\left(1-x_{1}-x_{2}\right) \mathrm{C}{6} \mathrm{H}{5} \mathrm{Cl}\right}) and the corresponding binary mixtures: (\quad\left{x \mathrm{C}{6} \mathrm{H}{6}+(1-x) c-\mathrm{C}{6} \mathrm{H}{12}\right}, \quad\left{x \mathrm{C}{6} \mathrm{H}{6}+(1-x) \mathrm{C}{6} \mathrm{H}{5} \mathrm{Cl}\right}), and (\left{x c-\mathrm{C}{6} \mathrm{H}{12}+(1-x) \mathrm{C}{6} \mathrm{H}{5} \mathrm{Cl}\right}), have been determined experimentally as a function of the mole fraction(s) at atmospheric pressure. Speeds of sound and densities were determined by density and sound analyzer Anton-Paar DSA-48 and refractive indices by the automatic refractometer ABBEMAT-HP Dr Kernchen. Variable-degree polynomials have been fitted to the results.

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