Speeds of sound, excess molar volumes, and isentropic compressibilities of “xCH3COC2H5 + (1 − x)C6H6’, “xCH3COC2H5 + (1 − x)C6H5CH3’, “xCH3COC2H5 + (1 − x)C6H5Cl’, and “xC2H5COC2H5 + (1 − x)C6H6’ at 298.15 K
✍ Scribed by Kazuyoshi Ohomuro; Katsutoshi Tamura; Sachio Murakami
- Publisher
- Elsevier Science
- Year
- 1987
- Tongue
- English
- Weight
- 314 KB
- Volume
- 19
- Category
- Article
- ISSN
- 0021-9614
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📜 SIMILAR VOLUMES
Speeds of sound u of {xC2H5OC2H5+(1-x)C6H6} and {xC2H5OC2H5+(1-x)CCl4} have been measured at T=298.15 K. Values of u have been used to calculate the isentropic compressibilities kS for these mixtures. The values of the excess isentropic compressibilities k E S have also been calculated and are found
Speeds of sound, densities, refractive indices, and isentropic compressibilities, at the temperature \(298.15 \mathrm{~K}\) of \(\left\{x_{1} \mathrm{C}_{6} \mathrm{H}_{6}+x_{2} \mathrm{c}-\mathrm{C}_{6} \mathrm{H}_{12}+\left(1-x_{1}-x_{2}\right) \mathrm{C}_{6} \mathrm{H}_{5} \mathrm{Cl}\right\}\) a