Excess molar volumes V E m of the ternary mixture {x1CH3(CH2)3OH+x2CH3(CH2)4CH3 + (1-x1-x2)CH3(CH2)3NH2} at the temperatures 298.15 K and 313.15 K, and the binary mixtures {xCH3(CH2)3OH + (1-x)CH3(CH2)3NH2}, {xCH3(CH2)4CH3 + (1-x)CH3(CH2)3NH2} at T=313.15 K have been determined from density measurem
Densities, speeds of sound, and isentropic compressibilities of binary and ternary mixtures containing CH3(CH2)3OH, CH3(CH2)4CH3, and CH3(CH2)3NH2at a temperature of 298.15 K
✍ Scribed by M. Domı́nguez; M.C. López; J. Santafé; F.M. Royo; J.S. Urieta
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 289 KB
- Volume
- 29
- Category
- Article
- ISSN
- 0021-9614
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✦ Synopsis
Densities r and speeds of sound u have been measured for {x1CH3(CH2)3OH + x2CH3(CH2)4CH3 + (1-x1-x2)CH3(CH2)3NH2}, and the corresponding mixtures CH2)3NH2}, at T = 298.15 K. Using these results, the isentropic compressibilities kS, the excess isentropic compressibilities k E S , and the speed of sound deviations Du, have been calculated for both the binary mixtures and the ternary system. Excess isentropic compressibilities and the speed of sound deviations have been fitted with the Redlich-Kister equation in the case of binary mixtures, while Cibulka's equation was used to fit the values relating to the ternary system.
📜 SIMILAR VOLUMES
Viscosities of a ternary mixture containing CH COOCH , CH OH, and CH CH CH OH at T s 298.15 K and atmospheric pressure have been measured over the whole range of mixture compositions. Viscosity deviations and excess molar Gibbs energy of activation of flow for the ternary system were calculated and
Excess molar volumes at the temperature 298.15 K were measured for , and {xCH3(CH2)4 CH3 +(1x)CH3(CH2)3OH}. Excess molar volumes were determined using an Anton Paar DMA 60/602 densimeter. The experimental values obtained in this work were compared with results obtained using methods which estimate
## Excess molar volumes at CH2 )n-2CH3}, (n= 10 or n = 12), and {xCH3(CH2)3CH2Cl + (1x)CH3(CH2)n-2CH3}, (n= 10 or n = 12), were determined using a densimeter Anton Paar DMA 60/602. All the experimental values were compared with the results obtained by empirical expressions for estimating ternar