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1.
Excess enthalpies, and heat capacities derived therefrom, have been obtained between 25 and 65 or 75°C at a constant concentration for cyclohexane and octamethylcyclotetrasiloxane mixed with normal hexadecane and with a highly branched C16 isomer, 2,2,4,4,6,8,8-heptamethylnonane, and also forcis-andtrans-decalin mixed withn-C16. Theh E values withn-C16 are positive and much larger than with the branched-C16. They decrease rapidly withT so thatc p E is large and negative. These results imply the presence of orientational order in then-C16, which is destroyed on mixing with the other component and which decreases withT. Theh E fortrans-decalin+n-C16 is much smaller than forcis-decalin+n-C16, and becomes negative with increase ofT. This change of sign, which is unexplained by current theory, is interpreted as due to an interference of the flat, plateliketrans-decalin molecule with the molecular motion of then-C16 chain.  相似文献   

2.
The pressure dependence of the excess enthalpy H E , dH E /dP, has been calculated from experimental excess volumes V E and dV E /dT using dH E /dP=V E –TdV E /dT. dH E /dP at zero pressure are reported at 25°C and equimolar concentration for the mixtures: cyclohexane with the series of normal alkanes (n-C n , where n=6,8,10,12,14 and 16) and with the series of highly branched alkanes (br-C n , where n=6,8,12 and 16), benzene, toluene and p-xylene +n-C n and 1-chloronaphthalene +n-C n and br-C n . Experimental and Flory theory dH E /dP values are in good agreement for the whole cyclohexane +br-C n series. For the n-C n series, dH E /dP becomes increasingly positive deviating from the Flory predictions. This discrepancy is due to the presence of short-range orientational order in the higher n-C n pure liquids which makes dH/dP more negative and which, upon mixing, is destroyed producing a positive contribution to dH E /dP not accounted for by the theory. The discrepancy between theoretical and experimental dH E /dP is large for benzene, but progressively smaller for toluene, p-xylene and 1-chloronaphthalene. These results are consistent with creation of order between the aromatic plate-like molecule and the long n-C n in solution. For 1-chloronaphthalene +n-C n , this order creation process produces a negative contribution to dH E /dP which balances the positive order-destruction contribution originated by the rupture, upon mixing, of short-range orientational order in pure n-C n .  相似文献   

3.
Using the Picker flow calorimeter, excess molar enthalpies H E have been obtained at 25°C for mixtures of 1,2-, 1,3- and 1,4-cis- and trans-dimethylcyclohexane and cis- and trans-decalin with n-hexadecane and the highly branched C16 isomer, 2,2,4,4,6,8,8-heptamethylnonane. Values of H E are also obtained for cis- and trans-decalin mixed with C6, C7, and C9 isomers. Anomalously low values of H E occur for normal alkanes mixed with cycloalkanes in the di-equatorial configuration, suggesting the presence of a negative contribution in H E possibly due to a restriction of n-alkane molecular motion by the flat, plate-like cycloalkane.  相似文献   

4.
Molar excess volumes V E at 25°C have been determined by vibrating-tube densimetry, as a function of mole fraction x for different series of an alkanoate (H 2m+1 C m COOC n H 2n+1 )+cyclohexane. Three types of alkanoates were investigated, i.e., methanoates (m=0, with n=3 and 4), ethanoates (m=1, with n=2, 3, and 4) and propanoates (m=2, with n=1, 2, and 3). In addition, a Picker flow calorimeter was used to obtain molar excess heat capacities C p E at constant pressure at the same temperature. V E is positive for all systems and rather symmetric, with V E (x=0.5) amounting to almost identical values in a series of mixtures containing an alkanoate isomer of same formula (say C4H8O2, C5H10O2, or C6H12O2). The composition dependence of C p E is rather unusual in that two more or less marked minima are observed for most of the mixtures, especially when the alkanoate is a methanoate or an ethanoate. These results are discussed in terms of possible changes in conformation of both the ester and cyclohexane.  相似文献   

5.
Molar excess mixing enthalpies h E , Gibbs free energies g E and hence entropies s E have been obtained using calorimetry and the vapor sorption method at 25°C for hexane isomers+2,2,4,4,6,8,8-heptamethylnonane, a highly branched C 16 . The h E and g E are negative while Ts E are positive, but small. The values are explained by the Prigogine-Flory theory through negative free volume contributions to h E and Ts E , counterbalanced in the case of Ts E by the positive combinatiorial Ts E for mixing molecules of different size. No contribution is seen from the interaction between methyl and methylene groups. The excess quantities are also obtained for hexane and heptane isomers mixed with n-hexadecane. Values of h E and Ts E are now strongly positive, while those of g E are only slightly less negative. The interpretation requires two recently advanced contributions in addition to those of the Prigogine-Flory theory: 1) a decrease of order when correlations of orientations between n-C 16 molecules in the pure liquid are replaced in the solution by weaker correlations whose strengths depend on the shapes of the lower alkane isomers. For lower alkane isomers of the same shape, but highly sterically hindered, h E and Ts E are small, manifesting, 2) a negative contribution, ascribed to a rotational ordering of n-C 16 segments on the sterically-hindered molecule. Enthalpy-entropy compensation is observed for these new contributions, arising from their rapid fall-off with increase of temperature.  相似文献   

6.
The excess volumes and enthalpies of mixing of binary mixtures of ethyl iodide with benzene, toluene, o-xylene, m-xylene and p-xylene have been measured experimentally over the whole composition range at 25°C. Qualitatively the data have been explained on the basis of electron donoracceptor interactions between the ethyl iodide and aromatic hydrocarbons and also on the loss of favorable orientational order of the pure components. Flory's theory correctly predicts the sign and to some extent magnitude of the V E and H E values.  相似文献   

7.
Densities have been obtained as a function of composition for ternary-pseudobinary mixtures of [(benzene + tetrachloromethane or n-hexane) + (cyclohexane + tetrachloromethane or n-hexane)] at atmospheric pressure and the temperature 298.15 K, by means of a vibrating-tube densimeter. Excess molar volumes, VmE, partial molar volumes and excess partial molar volumes were calculated from the density data. The values of VmE have been correlated using the Redlich–Kister equation and the coefficients and standard errors were estimated. The experimental and calculated quantities are used to discuss the mixing behavior of the components. The results show that the third component, CCl4 or n-C6H14, have quite different influences on the volumetric properties of binary liquid mixtures of benzene with cyclohexane.  相似文献   

8.
9.
In continuation of our work on excess thermodynamic properties of non-electrolyte solutions containing pyridine bases withn-alkanes, we have determined excess molar volumesV E for 2,4-dimethylpyridine + C6 to C10 n-alkanes at 25°C. For the investigated systems noV E values were available in the literature for comparison with our data. The experimentalV E was used to test the Prigogine-Flory-Patterson theory (PFP), Extended Real Associated Solutions model (ERAS) and the Treszczanowicz-Benson method (TB).  相似文献   

10.
The excess molar volumes V m E of binary mixtures of cyclohexane with several isomers of hexanol were measured at 25°C as a function of composition using a vibrating-tube digital densimeter. For all the systems V m E is positive over the entire range of mole fractions. Variable-degree polynomials have been fitted to the experimental results.  相似文献   

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