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 compress
Speeds of sound and isentropic compressibilities of {xCH3O(CH2)2OH+(1−x)H(CH2)ν(OCH2CH2)2OH} (ν=1, 2, and 4) at the temperature 298.15 K
✍ Scribed by A. Pal; W. Singh
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 209 KB
- Volume
- 29
- Category
- Article
- ISSN
- 0021-9614
No coin nor oath required. For personal study only.
✦ Synopsis
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 from a previous paper and combined with the measured values of the ultrasonic speeds to give estimates of the product KS,m of the molar volume and the isentropic compressibility kS, and the excess quantity K E S,m . The deviations of the speeds of sound u D were compared with the mixing function du calculated in the paper. The behaviour of u, u D , du, and K E S,m with composition and number of carbon atoms in the aliphatic chain of the alkoxyethanol is discussed.
📜 SIMILAR VOLUMES
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
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 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
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 sou
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