High pressure raman study of isotropic lineshapes of aqueous sodium nitrate solutions

The isotropic lineshape of the v₁ (A₁) stretching mode of the nitrate ion in solutions of sodium nitrate has been studied at 25°C as a function of NaNO₃ concentration ranging from 0.1 to 6M. The pressure dependence has been determined for 1 and 6M solutions at pressures ranging from 1 bar to 3 kbar. The isotropic band becomes more asymmetric with increasing concentration, and its v₁ peak frequency undergoes a blue shift both with increased concentration and increased pressure. At low concentration the vibrational correlation function is well described by the Kubo formula, whereas at higher concentration it becomes more Gaussian. The experimental data indicate that the v₁ vibrational lineshape in aqueous solutions of NaNO₃ is dominated by strong intermolecular interactions which produce inhomogeneous broadening at higher concentration.     

Thermal decomposition of aqueous manganese nitrate solutions and anhydrous manganese nitrate. Part 3. Isothermal kinetics

The kinetics of the thermal decomposition of aqueous manganese nitrate solutions and anhydrous manganese nitrate in air were established from isothermal experiments. By heating the solution, first most of the water evaporates to a composition of equimolar amounts of water and manganese nitrate; this concentrated solution then decomposes to γ-Mn(NO₂, NO₂ and water, usually in two steps. The first step can be described best by the model [?ln(1 ? α)]^{$\text{1}\text{2}$} = 8.9 × 10¹¹ exp(?121000/RT)t, whereas the second step is described equally well by several models. The kinetic parameters of these models are quite similar, the average activation energy being 141 kJ mole^?1.The decomposition of anhydrous Mn(NO₃)₂, which proceeds in a single step, can also be described with several similar models. In this case the average activation energy is about 92 kJ mole^?1.     

Nature of the optical absorption spectra of the trapped electron in irradiated frozen water solutions

Conclusions The optical absorption spectra of the trapped electron were measured in irradiated glasslike solutions of NaOH, KOH, and NaClO₄ in H₂O and D₂O at — 196°. The same as at room temperature, the spectra are caused by a transfer of the charge to the solvent.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 9, pp. 1637–1639, September, 1966.     

Trapped hydrogen atoms in irradiated frozen solutions. Isotope effects

Isotope effects in the yields of H- and D-atoms in acid, neutral and alkaline matrices have been studied by EPR methods. In acid matrices the isotope effect is the same in UV- and X-irradiated matrices, but in neutral and alkaline matrices the effect is larger in UV-irradiated matrices. Furthermore, when the H- and D-atoms are formed by photobleaching of trapped electrons the isotope effect is strongly dependent on the wavelength of the bleaching light, increasing with increasing wavelenghts. The isotope effect in sulphuric acid matrices is dependent on the concentration of the acid. The observation are briefly discussed.     

Polythermal study of the salting-out of triethylamine from aqueous solutions with sodium nitrate

Visual-polythermal method was used to study, in the temperature range from ?17 to 25°C, the phase equilibria and critical phenomena in the ternary system constituted by sodium nitrate, water, and triethanolamine, in which the boundary binary system is characterized by stratification with a lower critical solution point.     

Reaction of serum albumin with dimethyl sulfoxide according to PMR spectra of frozen aqueous solutions

The reaction of human serum albumin (HSA) with dimethyl sulfoxide (DMSO) was studied by the PMR method according to the intensity of the proton signal of non-freezable water in the temperature range of 230–273°K. It was shown that the concentration of DMSO in the non-frozen liquid phase is much higher than should be expected for the simple eutectic. This is attributable to the binding of N molecules of DMSO with a molecule of HSA (at 270°K, N = 7–10). It was found that in the presence of DMSO, the amount of non-freezable water markedly increased, which is possibly due to a reaction between DMSO and proton-active centers of the protein through the intermediate water molecules.Translated from Teoreticheskaya i Ékperimental'naya Khimiya, Vol. 25, No. 1, pp. 104–108, January–February, 1989.     

Radiolysis of aqueous solutions of gadolinium nitrate

The specific effect due to Gd³⁺ ion on the radiolysis of aqueous nitrate solutions was determined by measurement of H₂, H₂O₂ and NO ₂ ^– radiolytic yields produced by gamma-irradiation of aerated and deaerated solutions of gadolinium, sodium and calcium nitrates in the concentration range of 10^–5 to 0.3M. Important O₂ consumption in aerated and O₂ evolution in deaerated Gd(NO₃)₂ solutions was found by radiolysis in comparison with the inert cations nitrates. In the former the Gd³⁺ ion generates an O₂ transporter producing an increase in the H₂O₂ yield and a decrease in the NO ₂ ^– yield, while in the latter it enhances the H₂ and NO ₂ ^– production with respect to the same nitrate concentration of the Na⁺ solutions.     

Raman spectra of glassy aqueous solutions

The Raman spectra of glassy LiCl and LiBr aqueous solutions are obtained in the OH (OD) stretching vibrational region. Spectral features are discussed in conjunction with those of amorphous ice and liquid water.     

Enthalpic relaxation in frozen aqueous trehalose solutions

Our object was to investigate the effect of annealing on the glass transition temperatures and enthalpic recovery of frozen aqueous solutions of trehalose. Trehalose solutions were subjected to differential scanning calorimetry wherein they were first cooled from room temperature to −60 °C, and heated to the annealing temperature, which ranged between −34 and −48 °C. Following isothermal annealing for the desired time period, the glass transition temperatures and the enthalpic recovery were determined in the final heating scan. Frozen unannealed trehalose solutions were characterized by two glass transition events. At a heating rate of 2 °C/min, the observed Tg₁′ and Tg₂′ were ∼−45 and −31 °C, respectively. Annealing resulted in an increase in the lower transition temperature, Tg₁′, while the higher transition temperature, Tg₂′, was unaffected. Enthalpic recovery due to annealing was associated only with Tg₂′. Annealing at −36 °C resulted in the highest value of Tg₁′ and the maximum enthalpic recovery. Irrespective of the heating rates, the magnitude of enthalpic recovery and Tg₁′ showed a similar trend (first an increase, followed by a decrease) as a function of annealing temperature. This suggests that annealing led to crystallization of ice and subsequently the system became maximally freeze-concentrated. Annealing, at temperatures higher than −36 °C, led to a reduction in enthalpic recovery associated with Tg₂′ and a lowering of Tg₁′. These observations are consistent with the hypothesis that the higher transition temperature coincides with the onset of ice melting. We have attempted to bridge two conflicting schools of thought regarding the origin of multiple glass transitions in frozen aqueous sugar solutions. The two glass transitions are attributed to the formation of two “populations” in the freeze-concentrated phase during “non-equilibrium” or rapid cooling—one, that is maximally freeze-concentrated and the other that contains a higher amount of water. The higher transition temperature also overlaps with the onset of ice melting.