The speed of sound u has been obtained at a frequency of 4 MHz in 4xCH3O(CH2)2OH + (1 -x)H( CH2)n (OCH2CH2)2OH5 for n = 1, 2, and 4 over the whole range of x at T = 298.15 K and atmospheric pressure, using a NUSONIC velocimeter based on the sing-around technique. The excess molar volumes were taken
Speeds of sound and isentropic compressibilities of {xH(CH2)νO(CH2)2O(CH2)2OH +(1 −x)H2O}, (ν= 1, 2, and 4) at the temperature 298.15 K
✍ Scribed by A. Pal; Y.P. Singh
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 434 KB
- Volume
- 28
- Category
- Article
- ISSN
- 0021-9614
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✦ Synopsis
The speeds of sound in {xH(CH2)n O(CH2)2O(CH2)2OH + (1-x)H2O} for n=1, 2, and 4 have been measured over the whole range of x at the temperature T=298.15 K. The molar isentropic compressibilities KS, m of these solutions were estimated from the products of the molar volume and the isentropic compressibility kS , and the excess values K E S, m were also calculated. The behaviour of the K E S, m curves for the series of mixtures is similar to that found previously for their excess molar volumes. Also, the deviations of the speeds of sound u D has been defined and calculated for all measured values of x. These values were compared with the mixing function du calculated in the literature. The behaviour of u D , du, and K E S, m with composition and the number of carbon atoms in the aliphatic chain of the alkoxyethanol is discussed.
📜 SIMILAR VOLUMES
The speeds of sound have been measured in {xH(CH2)n(OC2H4)2OH + (1x)(C4H9)2O} for n = 1, 2, and 4 as a function of mole fraction x at the temperature 298.15 K, using a sing-around technique, and at a frequency of 4 MHz. The excess molar volumes were taken from the literature and combined with the me
The excess molar volumes of {xCH3O(CH2)2OH+(1-x)H(CH2)nO(CH2)2O(CH2)2OH} for n = 1, 2, and 4 have been measured as a function of composition using a continuous-dilution dilatometer at the temperature T=298.15 K. The excess molar volumes are negative over the entire range of composition for the syste
The excess molar volumes V E m of {xCH3(CH2)3OH + (1x)H( CH2)n(OCH2CH2)3OH} for n = 1, 2, and 4 were determined as a function of mole fraction x using a continuous-dilution dilatometer at the temperature 298.15 K. The V E m values decreased as the alkyl chain length of the alkoxyethanol increased. E
## 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