Showing: 10 from total: 1718 publications
1631. EVOLVING FACTOR-ANALYSIS OF SYNCHRONOUS FLUORESCENCE-SPECTRA OF FULVIC-ACIDS IN THE PRESENCE OF ALUMINUM
SILVA, CSPCO ; DASILVA, JCGE ; MACHADO, AASC
in APPLIED SPECTROSCOPY, 1994, ISSN: 0003-7028,  Volume: 48, 
Article,  Indexed in: wos 
P-001-KA9
Abstract The variations observed in synchronous fluorescence spectra of aqueous solutions (pH = 4) of three fulvic acids (fua) upon variation of the concentration of Al3+ were analyzed by evolving factor analysis (EFA). 'rhe three fua samples were extracted from materials present in a pinewood soil: dry pine needles and the upper and lower soil horizons. The presence of Al3+ induces quenching and enhancement of bands in the synchronous fluorescence spectra, and concentration constraints are proposed for the EFA analysis that allow the calculation, on a self-modeling curve resolution basis, of the number of components that show linearly independent variations, their spectra, and corresponding concentration profiles. Simulated and experimental data sets of simple known compounds (catechol, caffeic acid, salicylic acid, and morin) were also studied as the first validation of the experimental and data treatment procedures.

1632. ADSORPTION OF MANNITOL AND SORBITOL ON GOLD(111)
SOTTOMAYOR, MJ ; SILVA, F
in JOURNAL OF ELECTROANALYTICAL CHEMISTRY, 1994, ISSN: 0022-0728,  Volume: 376, 
Article,  Indexed in: crossref, scopus, wos 
Abstract The adsorption of mannitol and sorbitol on Au(111) has been followed by differential capacity measurements. Results obtained for the adsorption of these polyalcohols in dilute solutions of HClO4 and NaClO4 showed that the adsorption process could be described by a Frumkin isotherm, the parameters of which were determined and discussed. The values of the standard Gibbs energy of adsorption suggest physical adsorption of mannitol and sorbitol, without the existence of specific interactions of the adsorbed molecules with gold. The values of the interaction parameters are negative in both electrolytes, indicating a net attractive interaction in the adsorbed layer. There are noticeable differences between the values of the standard Gibbs energy of adsorption and of the interaction parameter for the two polyols, which have been interpreted in terms of the conformational properties of the two isomers in the adsorbed layer.

1633. A VOLTAMMETRIC STUDY OF A SURFACE PHASE-TRANSFORMATION OF ADSORBED HPO4(2-) ANION ON AU(111) IN THE PRESENCE OF NA(+) CATIONS
SILVA, F ; SOTTOMAYOR, MJ ; MARTINS, A
in JOURNAL OF ELECTROANALYTICAL CHEMISTRY, 1994, ISSN: 1572-6657,  Volume: 375, 
Note,  Indexed in: crossref, scopus, wos 

1634. STUDY OF ELECTROCHEMICAL PROPERTIES OF AU(210) FACE ELECTRODE IN NITRATE SOLUTIONS
SILVA, F ; SOTTOMAYOR, MJ ; MARTINS, A
in ELECTROCHIMICA ACTA, 1994, ISSN: 0013-4686,  Volume: 39, 
Article,  Indexed in: crossref, scopus, wos 
Abstract The behaviour of Au(210) in HNO3 and NaNO3 solutions was studied with cyclic voltammetry and differential capacity measurements as a function of concentration and temperature. The effect of concentration on both j-E profiles and C(E) curves suggests that for low concentrations and around zero charge potential, NO3- adsorption is similar to ClO4- adsorption on Au(210). For higher concentrations, the adsorption of NO3- ions at positive charges seems to occur to a greater extent than ClO4- ions. The entropy of formation of the electrochemical interface was derived from the effect of temperature in HNO3 solution. It was found to be qualitatively similar to what was observed in HClO4, solution.

1635. VAPOR-PRESSURES AND STANDARD MOLAR ENTHALPY OF SUBLIMATION OF CRYSTALLINE TRIS(PENTANE-2,4-DIONATO)RUTHENIUM(III)
DASILVA, MAVR ; GIERA, E ; MONTE, MJS
in JOURNAL OF ALLOYS AND COMPOUNDS, 1993, ISSN: 0925-8388,  Volume: 197, 
Article,  Indexed in: scopus, wos 
P-001-MYQ
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.

1636. ENTHALPIES OF COMBUSTION, VAPOR-PRESSURES, AND ENTHALPIES OF SUBLIMATION OF 3-AMINOQUINOLINE, 5-AMINOQUINOLINE, 6-AMINOQUINOLINE, AND 8-AMINOQUINOLINE
DASILVA, MAVR ; MATOS, MAR ; MONTE, MJS ; ALVES, MCB ; VIEIRA, JMAP
in JOURNAL OF CHEMICAL THERMODYNAMICS, 1993, ISSN: 0021-9614,  Volume: 25, 
Article,  Indexed in: scopus, wos 
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]].

1637. SELF-ASSEMBLY IN MIXTURES OF A CATIONIC AND AN ANIONIC SURFACTANT - THE SODIUM DODECYL-SULFATE DIDODECYLDIMETHYLAMMONIUM BROMIDE WATER-SYSTEM
MARQUES, E ; KHAN, A ; MIGUEL, MD ; LINDMAN, B
in JOURNAL OF PHYSICAL CHEMISTRY, 1993, ISSN: 0022-3654,  Volume: 97, 
Article,  Indexed in: crossref, scopus, wos 
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.

1638. THERMOCHEMICAL AND THEORETICAL-STUDIES ON CYCLOHEXANEDIONES
PILCHER, G ; PARCHMENT, OG ; HILLIER, IH ; HEATLEY, F ; FLETCHER, D ; DASILVA, MAVR ; FERRAO, MLCCH ; MONTE, MJS ; JIYE, F
in JOURNAL OF PHYSICAL CHEMISTRY, 1993, ISSN: 0022-3654,  Volume: 97, 
Article,  Indexed in: crossref, scopus, wos 
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.

1639. PHASE-BEHAVIOR OF POLYMER-SURFACTANT SYSTEMS IN RELATION TO POLYMER-POLYMER AND SURFACTANT-SURFACTANT MIXTURES
LINDMAN, B ; KHAN, A ; MARQUES, E ; MIGUEL, MD ; PICULELL, L ; THALBERG, K
in PURE AND APPLIED CHEMISTRY, 1993, ISSN: 0033-4545,  Volume: 65, 
Article,  Indexed in: crossref, wos 
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.

1640. THE ENTHALPY OF SUBLIMATION OF DIPHENYLACETYLENE FROM KNUDSEN EFFUSION STUDIES
DIOGO, HP ; DAPIEDADE, MEM ; FERNANDES, AC ; SIMOES, JAM ; DASILVA, MAVR ; MONTE, MJS
in THERMOCHIMICA ACTA, 1993, ISSN: 0040-6031,  Volume: 228, 
Article,  Indexed in: crossref, scopus, wos 
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].