Temperature dependence of nonsteady dislocation-induced internal friction

A change in the number of weak pinning points results in the time dependence of the dislocation-induced internal friction. The paper considers the temperature dependence of the nonsteady component of the damping decrement Q^–1, induced by partial scattering of the cloud of point defects. There exists a temperature peak Q^–1(T), whose height and temperature vary as the frequency changes. The relation between the frequency, height, and temperature of the peak is considered. The results can be used to determine the character and type of weak pinning points.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 9, pp. 59–63, September, 1981.     

Influence of component ratio in the compound (Mg,Fe)3Si2O5(OH)4 on the formation of nanotubular and platelike particles

Organically modified layered magnesium silicate was for the first time synthesized by thermal treatment of a sol of silicon dioxide, magnesium hydroxide, and hexadecyl trimethylammonium bromide, with reflux of the liquid phase. The material obtained can be used as an ultradispersed component in polymer-inorganic composites.     

Mechanism of the decomposition of the surface oxide film on polycrystalline palladium

The decomposition of thin surface oxide films on polycrystalline palladium Pd(poly) at 500–1300 K was investigated by mathematical modeling. This process was analyzed in terms of a model including O₂ desorption from the chemisorbed oxygen layer (O_ads) and the passage of oxygen inserted under the surface layer of the metal (O_abs) and oxygen dissolved in metal subsurface layers (O_dis) to the surface. O₂ desorption was modeled on a surface with a square lattice of adsorption sites, with account taken of the energy of the lateral repulsive interactions between adjacent O_ads atoms (ε_aa). At ε_aa = 10 kJ/mol and when the activation energy of O₂ desorption for a chemisorbed-oxygen surface coverage of θ ≈ 0 is E_des⁰ = 230 kJ/mol, the calculated spectra are in agreement with the oxygen temperature-programmed desorption (TPD) spectra obtained for Pd(poly) at θ ≤ 0.5. The passage of O_abs and O_dis atoms to the surface was calculated using a first-order equation, with account taken of the activation energy for these atoms coming out to the surface (E₂ and E₃, respectively). As the oxide film is heated, O₂ desorption is accompanied by the passage of O_abs and then O_dis to the surface, which leads to an increase in the O_ads surface coverage and, accordingly, to a buildup of lateral surroundings in the adsorbed layer. Owing to this fact and to the repulsive interactions between O_ads atoms, the bonds between O_ads and the surface weaken and E_des decreases. As a consequence, the O₂ desorption rate increases and a low-temperature peak with T_max ≈ 710 K, which is due to the passage of O_abs atoms to the surface, and then a high-temperature peak with T_max ≈ 770 K, which is due to the passage of O_dis atoms to the surface, appear in the TPD spectrum. At ε_aa = 10 kJ/mol, E_des⁰ = 230 kJ/mol, E₂ = 145 kJ/mol, and E₃ = 160 kJ/mol and when the number of inserted oxygen monolayers is θ_abs ≤ 0.3 and the number of oxygen monolayers dissolved in subsurface layers is θ_dis ≤ 10, the TPD spectra calculated for the given model are in agreement with the O₂ TPD spectra that are observed for Pd(poly) and are due to the decomposition of surface oxide films.     

Interaction between oxygen and polycrystalline palladium at O<Subscript>2</Subscript> pressures of 10<Superscript>−6</Superscript>–10 Pa

The interaction between oxygen and polycrystalline palladium (Pd(poly)) at \(P_{O_2 } \) = 2.6 × 10^?6–10 Pa and T = 300–1300 K was studied by the thermal desorption (TD) method. The interaction between O₂ and Pd(poly) is governed by the O₂ pressure and the sample temperature. At low pressures of \(P_{O_2 } \) (≤1.3 × 10^?5 Pa), O₂ is chemisorbed dissociatively on the Pd(poly) surface. During chemisorption, the O_ads-surface bond energy and the O₂ sticking coefficient gradually decrease as the surface coverage θ increases. At \(P_{O_2 } \) ≥ 10^?2 Pa and T ≤ 500 K, after the saturation of the O_ads layer (θ ～ 0.5), O_ads atoms penetrate under the surface layer of the metal to form surface palladium oxide. At \(P_{O_2 } \) ≥ 1 Pa and T > 500 K, after the saturation of the surface oxide film 2 ML in thickness (n ～ 2), O_ads atoms penetrate into the oxide film and then into the subsurface palladium layer and diffuse deep into the metal bulk. As a result, the oxygen uptake at 700 K is n ～ 50. Upon heating, the surface oxides decompose, desorbing O₂, which gives rise to a low-temperature TD peak with T _max = 715 K. The release of oxygen inserted in the subsurface layers of palladium shows itself as a distinct high-temperature TD peak with T _max ≥ 750 K.     

The α-effect of oximate ions and solvent effect in the transfer of the toluenesulfonyl group in aqueous dimethylsulfoxide

The kinetic behaviour of oximate ions was studied in the transfer of the toluenesulfonyl group in aqueous dimethylsulfoxide (0–95 vol.% DMSO). The solvation effects of the solvent are a factor controlling the nucleophilicity and magnitude of the α-effect of the oximate ions. L. M. Litvinenko Institute of Physical Organic and Coal Chemistry, National Academy of Sciences of Ukraine, 70 R. Lyuksemburg ul., Donetsk 340114, Ukraine. Translated from Teoreticheskaya i éksperimental'naya Khimiya, Vol. 36, No. 1, pp. 30–35, January–February, 2000.     

Limit distribution of the position of a semicontinuous process with negative infinite mean at the moment of exit from an interval

Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 40, No. 4, pp. 538–541, July–August, 1988.