Publications

Abstract The Knudsen mass loss effusion technique was used to measure the vapour pressure of crystalline tris(pentane-2,4-dionato)ruthenium(III) as a function of temperature between 398.18 and 413.15 K using three different effusion holes. From the temperature dependence of the vapour pressure, the standard molar enthalpy of sublimation at the mean temperature of the experimental temperature range, 405.7 K, was derived as 139.7 +/- 2.5 kJ mol-1. Using an estimated value of DELTA(cr)gC(p)o = -50 J K-1 mol-1, the standard molar enthalpy of sublimation at 298.15 K was calculated as 145.1 +/- 2.5 kJ mol-1.

Abstract The standard (po = 0.1 MPa) molar enthalpies of formation for crystallin 3-, 5-, 6-, and 8-aminoquinoline were derived from the standard molar enthalpies of combustion, in oxygen, at the temperature T = 298.15 K, measured by static-bomb combustion calorimetry; the Knudsen mass-loss effusion technique was used to measure the vapour pressures of the crystals as functions of temperature, and the standard molar enthalpies of sublimation, at the temperature T = 298.15 K, were derived by the Clausius-Clapeyron equation. Direct measurements of the standard molar enthalpies of sublimation, using microcalorimetry, for 3- and 5-aminoquinoline, confirmed the values from the Knudsen technique. [[formula]].

Abstract The phase equilibria of the sodium dodecyl sulfate (SDS)-didodecyldimethylammonium bromide (DDAB)-water system have been studied by water deuteron NMR and polarizing microscopy methods at 40-degrees-C. H-1 NMR relaxation, PGSE FT-NMR self-diffusion, and dynamic light scattering are used to study aggregate structures of isotropic phases. A pseudoternary representation of the four-component phase diagram contains a large number of regions of homogeneous solutions and liquid crystalline phases, as well as multiphase regions. Isotropic solution regions contain SDS-rich micellar aggregates or (spontaneously forming) vesicles, rich in either surfactant; the vesicles form at very high dilution (<0.1% surfactant). Addition of DDAB to solutions of spherical SDS micelles may induce a micellar growth to rodlike aggregates. There is a large region of bicontinuous cubic liquid crystalline phase, with high concentrations of both surfactants. The phase diagram contains several regions of lamellar liquid crystalline phase, and under certain conditions two lamellar phases may coexist. The two lamellar phases of the binary DDAB-water system can incorporate very different amounts of SDS, the one dilute in DDAB only small amounts, but the concentrated one large amounts. In addition, the lamellar phase may form for concentrated roughly equimolar mixtures of the two surfactants and for mixtures containing high concentrations of SDS. The possible connection between different lamellar regions in an appropriate three (or higher) dimensional phase diagram is discussed as well as the interactions, in terms of electrostatic and molecular packing effects, giving rise to the observed phase behavior and solution microstructure.

Abstract The following standard molar enthalpies of formation in the gaseous state at 298.15 K were determined from the enthalpies of combustion of the crystalline solids and the enthalpies of sublimation: 1,3-cyclohexanedione, -335.6 +/- 1.6 kJ mol-1; 1,4-cyclohexanedione, -332.6 +/- 1.2 kJ mol-1; 4,4-dimethyl-1,3-cyclohexanedione, -400.4 +/- 2.7 kJ mol-1; and 5,5-dimethyl-1,3-cyclohexanedione, -383.6 +/- 1.9 kJ mol-1. Ab initio calculations were made of the enthalpies of isomerization of the three cyclohexanediones and of the isomerization of 1,3-cyclohexanedione to its enol forms: the keto form of 1,3-cyclohexanedione in the gaseous state was predicted to be energetically more stable than the enol form by 18.0 kJ mol-1. NMR spectra, however, showed the compound in the crystalline state to exist in the enol form with the molecules held together by intermolecular hydrogen bonds. The enthalpy of formation of 1,2-cyclohexanedione in the gaseous state, not amenable to experimental measurement, was predicted to be -300 +/- 5 kJ mol-1, and the conventional strain energies in the three cyclohexanedione isomers were estimated to be of similar magnitude, ca. 13 kJ mol-1.

Abstract Novel phase diagrams of systems of water and two cosolutes of colloidal size, either macromolecules or surfactant micelles, are presented. For a mixture of two oppositely charged surfactants, a complex phase diagram is obtained with several liquid crystalline phases and equilibrium vesicles. There is a strong tendency for two surfactants to mix and form a range of structures governed by geometrical packing and electrostatic interactions. In recent years, surfactant self-assembly in the presence of different polymers has attracted a great interest, both from fundamental and applied aspects. Attractive or repulsive interactions are observed depending on the system. For the former case, dilute solutions may be analysed in terms of a binding of the surfactant to the polymer or a depression of the critical micelle concentration of the surfactant by the polymer. An important feature of these solutions is thus that the surfactant molecules, also when interacting intimately with a polymer, give micellar-type structures. The phase behavior of polymer-surfactant systems has only recently attracted greater attention but has been shown most significant for the understanding of the interactions involved. Different types of phase separation phenomena are encountered including segregative and associative types. For systems of a polyelectrolyte and an oppositely charged surfactant, an associative interaction is observed leading to phase separation into one solution concentrated in both polymer and surfactant and one very dilute solution. In the presence of an electrolyte, phase separation may be eliminated and, at higher concentrations, a polymer incompatibility type of phase separation may result. It is found fruitful to analyse the phase diagrams of polymer-surfactant systems with those of polymer-polymer and surfactant-surfactant mixtures as a basis. Analogies and differences are discussed and it is found that polymer-surfactant systems show basic similarities to polymer-polymer systems, while surfactant mixtures are different, which is due to the exchange of surfactant molecules between micelles and the formation of mixed micelles and other aggregates. Surfactant mixtures are, therefore, not displaying a segregative type of phase separation.

Abstract The enthalpy of sublimation of diphenylacetylene at 298.15 K, DELTA(cr)g H(m)THETA (C2(C6H5)2] = 95.1 +/- 1.1 kJ mol-1, was derived from vapour pressure-temperature data, obtained with two different Knudsen effusion apparatus, and from heat capacity measurements obtained by differential scanning calorimetry. The molybdenum-diphenylacetylene bond dissociation enthalpy in Mo(eta5-C5H5)2[C2(C6H5)2] was reevaluated as 115 +/- 26 kJ mol-1, on the basis of the new value for DELTA(cr)g H(m)THETA C2(C6H5)2].

Abstract The standard (po = 0.1 MPa) molar enthalpy of formation, at the temperature 298.15 K, of crystalline bis(2,2,6,6-tetramethylheptane-3,5-dionato) dioxouranium(VI) {uranyl(VI) dipivaloylmethanate, UO2(DPM)2}, was determined by solution-reaction calorimetry as -(2169.9±7.6) kJ·mol-1. The vapour pressure of the crystal, as function of the temperature, was measured using the Knudsen mass-loss effusion technique and the standard molar enthalpy of sublimation, at the temperature 298.15 K, was derived as (156.9±1.9) kJ·mol-1. From these results, the standard molar enthalpy of formation of the complex, in the gaseous state, was derived and the mean uranium(VI)-oxygen bond-dissociation enthalpy for the binding of the ligand to the metal, 〈D〉(U-O), was calculated as (223±10) kJ·mol-1.

Abstract The standard (po = 0.1 MPa) molar enthalpies of combustion at the temperature T = 298.15 K were measured by static-bomb calorimetry for crystalline 2,2′,4,4′,6,6′-hexamethylazobenzene-N,N-dioxide (HHMABOO), 2,2′,6,6′-tetramethylazobenzene-N,N-dioxide (TMABOO), 2,4,6-trimethylnitrobenzene (NITME), and liquid 2,6-dimethylnitrobenzene (NITXY). The enthalpies of sublimation at the temperature 298.15 K of HMABOO and TMABOO were assessed from vapour-pressure measurements; the enthalpy of sublimation of NITME and the enthalpy of vaporization of NITXY were measured by microcalorimetry. The standard molar enthalpies of decomposition of the crystalline N,N -dioxides to the corresponding gaseous monomeric nitroso-compounds at T = 298.15 K were measured by microcalorimetry: for HMABOO, (181.1±2.5) kJ·mol-1, and for TMABOO, (179.2±2.2) kJ·mol-1. For HMABOO and TMABOO, D (N=N)/(kJ·mol-1) was derived as (74.1±12.2) and (72.2±12.2), and 〈D(N-O&gt;〉/(kJ·mol-1) as (285.7±6.8) and (287.8±6.6), respectively. D (N-O)/(kJ·mol-1) in NITME and in NITXY was derived as (383.4±2.9) and (380.4±2.3), respectively.

Abstract The standard (po = 0.1 MPa) molar enthalpies of combustion at the temperature 298.15 K were measured by static-bomb calorimetry for p -azoxyanisole and p-azoxyphenetole, and the standard molar enthalpies of sublimation of the temperature 298.15 K were measured by microcalorimetry. [[formula]] From the standard the molar enthalpies of formation of the gaseous compounds, the molar dissociation enthalpies of the N-O bonds were derived: D (N-O)/(kJ·mol-1): p-azoxyanisole, 317.2±5.7; p-azoxyphenetole, 320.4±4.9. Microcalorimetric measurements were made to derive the molar enthalpies of the transitions: crystal-to-liquid: for p-azoxyanisole, (29.3±0.8) kJ·mol-1, (1.0±0.5) kJ·mol-1; and for p-azoxyphenetole, (27.0±0.8) kJ·mol-1, (1.7±0.6) kJ·mol-1, respectively.