𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Ultrasonic speeds and isentropic functions of [2-{2-(2-alkoxyethoxy)ethoxy}ethanol + di-n-butylether] at the temperature 298.15 K

✍ Scribed by Amalendu Pal; Sanjay Sharma


Publisher
Elsevier Science
Year
1998
Tongue
English
Weight
184 KB
Volume
30
Category
Article
ISSN
0021-9614

No coin nor oath required. For personal study only.

✦ Synopsis


w Γ„ Ε½ . 4 Ultrasonic speeds u have been measured in 2-2-2-methoxyethoxy ethoxy ethanol q dix w Γ„ Ε½ . 4

x w Γ„ Ε½ n-butylether , 2-2-2-ethoxyethoxy ethoxy ethanol q di-n-butylether , and 2-2-2-. 4

x butoxyethoxy ethoxy ethanol q di-n-butylether systems across the entire composition ranges, at the temperature 298.15 K, using a sing-around technique, at a frequency of 4 MHz. The values have been combined with those of the excess molar volumes to obtain estimates of the product K of the molar volume and the isentropic compressibility , and the excess

S, m S

values K E were also calculated. The deviation u D of the ultrasonic speeds from their

values in an ideal mixture were also evaluated for all measured values of x. These values are compared with the mixing function ␦ u calculated in the paper. The behaviour of u, u D , and K E with composition and the number of carbon atoms in the aliphatic chain of the S, m alkoxyethanol is discussed.


πŸ“œ SIMILAR VOLUMES


Ultrasonic speeds and volumetric propert
✍ A. Pal; S. Sharma; G. Dass πŸ“‚ Article πŸ“… 1999 πŸ› Elsevier Science 🌐 English βš– 178 KB

The excess molar volume and ultrasonic speed of (polyethers + 2-methoxyethanol) have been measured at the temperature 298.15 K as a function of composition. The polyethers were ethylene glycol dimethyl ether, diethylene glycol dimethyl ether, triethylene glycol dimethyl ether, diethylene glycol diet

Speeds of sound and isentropic compressi
✍ A. Pal; Y.P. Singh πŸ“‚ Article πŸ“… 1996 πŸ› Elsevier Science 🌐 English βš– 434 KB

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

The speed of sound and isentropic functi
✍ A. Pal; Y.P. Singh πŸ“‚ Article πŸ“… 1996 πŸ› Elsevier Science 🌐 English βš– 216 KB

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

Speeds of sound and isentropic compressi
✍ A. Pal; W. Singh πŸ“‚ Article πŸ“… 1997 πŸ› Elsevier Science 🌐 English βš– 209 KB

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

Densities, speeds of sound, and isentrop
✍ M. DomΔ±́nguez; M.C. LΓ³pez; J. SantafΓ©; F.M. Royo; J.S. Urieta πŸ“‚ Article πŸ“… 1997 πŸ› Elsevier Science 🌐 English βš– 289 KB

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

Speeds of sound, densities, refractive i
✍ M. Iglesias; B. Orge; J. Tojo πŸ“‚ Article πŸ“… 1994 πŸ› Elsevier Science 🌐 English βš– 159 KB

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