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Speeds of sound in and isentropic compressibilities of (1,1,2,2,-tetrachloroethane + anisole, 1,4-dioxane, methylethylketone, and pyridine) atT= 303.15 K

โœ Scribed by Jagan Nath


Publisher
Elsevier Science
Year
1996
Tongue
English
Weight
213 KB
Volume
28
Category
Article
ISSN
0021-9614

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โœฆ Synopsis


Measurements of speeds of sound u have been made in binary mixtures of 1,1,2,2-tetrachlorethane (CHCl2CHCl2) with anisole (C6H5OCH3), 1,4-dioxane (C4H8O2), methylethylketone (CH3COC2H5), and pyridine (C5H5N) at T = 303.15 K. Values of u have been used to calculate the apparent excess speeds of sound Du and the isentropic compressibilities kS for these mixtures. The excess isentropic compressibilities k E S have also been calculated from the values of kS. The k E S have been found to be highly negative for {xCHCl2CHCl2 + (1x)CH3COC2H5}, and very slightly negative for {xCHCl2CHCl2 + (1x)C4H8O2}. The k E S is very slightly negative at low x, and very slightly positive at higher x for {xCHCl2CHCl2 + (1-x)C6H5OCH3}. The k E S is also very slightly negative for {xCHCl2CHCl2 + (1-x)C5H5N} at low x and, compared with {xCHCl2CHCl2 + (1x)C6H5OCH3}, the k E S is more positive for {xCHCl2CHCl2 + (1x)C5H5N} at higher x. Values of k E S for the various systems have been discussed in the light of interactions between the components.


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Excess molar volumes V E m and speeds of sound u were measured for {1,4-dioxane The values of u for the various mixtures were used to calculate the apparent excess speeds of sound u and the isentropic compressibilities ฮบ S . The excess isentropic compressibilities ฮบ E S have also been calculated fr

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Measurements of speeds of sound u have been made in binary liquid mixtures of cyclohexanone (C 6 H 10 O) and dichloromethane (CH 2 Cl 2 ), or trichloromethane (CHCl 3 ), or trichloroethene (CHClCCl 2 ), or 1,2-dichloroethane (CH 2 ClCH 2 Cl) at T = 303.15 K. The values of u have been used to calcula