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Abstract  

The authors have measured the vapour pressure of the binary systems, piperidine+n -butylamine, piperidine+dipropylamine, piperidine+N-methyl piperidine, piperidine+N,N-dimethyl amino butane and N-methyl piperidine+n -butylamine. The measurements were carried out using an isoteniscope built by Jose [1]. The vapour pressure, excess Gibbs free energies at 298,15, 303,15, 313,15, 323,15, 333,15, and 325,15 K, are reported for these mixtures. The excess Gibbs free energies have been fitted to Redlich-Kister equation.

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The authors have measured the vapour pressure of the four binary systems, piperidine +tert-butyl methyl ether, piperidine +1,4 dioxane, piperidine + tetrahydropyrane and N-methyl piperidine +tert-butyl methyl ether. The measurements were carried out using an isoteniscope built by J. Jose [1], The vapour pressure, excess Gibbs free energies at 298.15, 303.15, 313.15, 323.15, 333.15 and 343.15 K, are reported for these mixtures. The excess Gibbs free energies have been fitted to the Redlich-Kister equation.

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Abstract  

Densities, speeds of sound and refractive indices of the binary mixtures 1,3-dioxolane or 1,4-dioxan+1-chloropentane or 1-chlorohexane have been measured at the temperatures of 298.15 and 313.15 K. Excess molar volumes, isentropic compressibilities, isentropic compressibility deviations and refractive index deviations have been obtained from experimental data. Excess molar volumes, isentropic compressibility and refractive index deviations have been fitted to a Redlich-Kister equation. Excess molar volumes, speeds of sound and isentropic compressibilities have been estimated at 298.15 K using the Prigogine-Flory-Patterson theory.

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Abstract  

The authors have measured the vapour pressure of four binary systems, morpholine+piperidine, morpholine+1,4-dioxane, morpholine+tetrahydropyrane and 1,4-dioxane+tetrahydropyrane. The measurements were carried out using an isoteniscope built by J. Jose [1]. The vapour pressure, excess Gibbs free energies at 298.15, 303.15, 313.15, 323.15, 333.15 and 343.15 K are reported for these mixtures. The excess Gibbs free energies have been fitted to the Redlich-Kister equation.

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Abstract  

The authors have measured the vapour pressure of the binary four systems, piperidin +1,4-dioxan, piperidin+tetrahydropyran, piperidin+tert-butyl methyl ether and N-methyl piperidin+tert-butyl methyl ether. The measurements were carried out using an isoteniscope built by J. Jose [1]. The vapour pressure, excess Gibbs free energies at 298.15 K, 303.15 K, 313.15 K, 323.15 K, 333.15 K and 343.15 K, are reported for these mixtures. The excess Gibbs free energies have been fitted to the Redlich-Kister equation.

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Excess molar enthalpies of dichloropropane + n-alkane mixtures

Study on the effect of increasing the chain length of the n-alkane and the influence of the chlorine position

Journal of Thermal Analysis and Calorimetry
Authors: M. Mato, J. Fernández, J. Legido, and M. Paz Andrade

Abstract  

We have determined the excess molar enthalpies
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at 298.15 K and normal atmospheric pressure for the binary mixtures containing dichloropropane and n-alkane [{xCH2ClCHClCH3 + (1−x) CnH2n+2 (n = 6, 8, 10, 12)} and {xCH2ClCH2CH2Cl + (1−x) CnH2n+2 (n = 8, 10)}] using a Calvet microcalorimeter. The
\documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{upgreek} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} $$H_{\text{m}}^{\text{E}}$$ \end{document}
values for all the mixtures show endothermic behaviour for the whole composition range. The Redlich–Kister equation was used to correlated the experimental values. The experimental excess molar enthalpies were examined on basis of the DISQUAC group-contribution model and the UNIFAC group-contribution method using the version considered by Larsen et al. The experimental and calculated results are discussed in terms of molecular interactions and the proximity effect.
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The excess enthalpies were investigated for 12 binary and 4 ternary systems, including mixtures and solutions of electrolytes and non-electrolytes. The excess enthalpies of mixtures and integral heats of solutions were measured with an isoperibol calorimeter at 35 °C. Heats of fusion and heat capacities as functions of temperature were measured with a Perkin Elmer Corp., DSC-2. Integral heats, heats of fusion and heat capacities allow investigations of excess enthalpies of solutions. For modelling of the experimental results, the modified Redlich-Kister equation was used with good success.

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experimental Y E ( Y = H or V ) data of the binary mixtures containing EAN or PAN (1) with water (2), reported in Table 2 , were fitted to the smoothing Redlich–Kister equation: (4) with 3 or 4 parameters, were x 1 is the mole fraction of the RTILs

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Journal of Thermal Analysis and Calorimetry
Authors: B. Marongiu, Silvia Porcedda, D. Falconieri, Alessandra Piras, E. Matteoli, and L. Lepori

energies, G E , have been obtained by reduction with the two or three parameters Redlich–Kister equation of the direct experimental isothermal P , x or P , x , y data [ 17 ]. Vapor phase imperfection was accounted for in terms of the second virial

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