Pub Date : 2025-03-18DOI: 10.1134/S0020168525700062
A. A. Burkov, M. A. Kulik
Nickel and aluminum powders have been deposited for the first time on steel 35 by electrospark deposition. We have studied the effect of the ratio of the Ni and Al powders in the anodic mixture on the structure, oxidation resistance, and corrosion behavior of the coatings and also on their friction coefficient and wear resistance. The results demonstrate that, as the fraction of aluminum powder in the anodic mixture increases from 30 to 70 at %, the average aluminum content of the coatings increases steadily from 39 to 63 at %, whereas the nickel content decreases from 46 to 26 at %. The use of such coatings allows the oxidation resistance of steel 35 parts at a temperature of 700°C to be raised 13 to 34 times. The most aluminum rich coating has been shown to have the highest hardness, wear resistance, and heat resistance.
{"title":"Structure, Oxidation Resistance, and Corrosion and Tribological Characteristics of Coatings Produced by Electrospark Deposition of Ni and Al Powders on Steel 35","authors":"A. A. Burkov, M. A. Kulik","doi":"10.1134/S0020168525700062","DOIUrl":"10.1134/S0020168525700062","url":null,"abstract":"<p>Nickel and aluminum powders have been deposited for the first time on steel 35 by electrospark deposition. We have studied the effect of the ratio of the Ni and Al powders in the anodic mixture on the structure, oxidation resistance, and corrosion behavior of the coatings and also on their friction coefficient and wear resistance. The results demonstrate that, as the fraction of aluminum powder in the anodic mixture increases from 30 to 70 at %, the average aluminum content of the coatings increases steadily from 39 to 63 at %, whereas the nickel content decreases from 46 to 26 at %. The use of such coatings allows the oxidation resistance of steel 35 parts at a temperature of 700°C to be raised 13 to 34 times. The most aluminum rich coating has been shown to have the highest hardness, wear resistance, and heat resistance.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 11","pages":"1327 - 1336"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645399","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701371
I. I. Buchinskaya, P. A. Popov, N. I. Sorokin
A single crystal of a Pb1−xScxF2+x heterovalent solid solution with x = 0.1 (nominal composition) has been grown by vertical directional solidification (Bridgman technique), its elemental and phase compositions and crystallographic parameters have been determined, and the interrelation between its thermal and electrical conductivities has been analyzed. The composition of the solid solution has been found to vary from x = 0.08 in the bottom (cone) of the crystal to x = 0.095 in its top. The Pb1−xScxF2+x crystal has been shown to have low thermal conductivity (k = 0.7 W/(m K) at 300 K), with “glass-like” behavior of thermal transport, atypical of the crystalline state, in combination with high fluoride ion electrical conductivity (σdc = 0.012 S/m at 293 K) and relatively low activation enthalpy for electrical conduction (ΔHσ = 0.378 ± 0.005 eV). The observed behavior of the thermal and electrical conductivities of the Pb1−xScxF2+x solid solution is due to structural disorder in the fluorine sublattice—which persists at room temperature—as a result of heterovalent substitutions of Sc3+ for Pb2+ cations. The thermal and electrical conductivities of single crystals of Pb1−xScxF2+x and Pb1−xCdxF2 two-component solid solutions (CaF2 structure) are compared to those of the β-PbF2 (CaF2 structure) and ScF3 (ReO3 structure) single-component fluorides.
{"title":"Crystal Growth of a Pb1−xScxF2+x Superionic Conductor and Investigation of the Interrelation between Its Thermal and Electrical Conductivities","authors":"I. I. Buchinskaya, P. A. Popov, N. I. Sorokin","doi":"10.1134/S0020168524701371","DOIUrl":"10.1134/S0020168524701371","url":null,"abstract":"<p>A single crystal of a Pb<sub>1−<i>x</i></sub>Sc<sub><i>x</i></sub>F<sub>2+<i>x</i></sub> heterovalent solid solution with <i>x</i> = 0.1 (nominal composition) has been grown by vertical directional solidification (Bridgman technique), its elemental and phase compositions and crystallographic parameters have been determined, and the interrelation between its thermal and electrical conductivities has been analyzed. The composition of the solid solution has been found to vary from <i>x</i> = 0.08 in the bottom (cone) of the crystal to <i>x</i> = 0.095 in its top. The Pb<sub>1−<i>x</i></sub>Sc<sub><i>x</i></sub>F<sub>2+<i>x</i></sub> crystal has been shown to have low thermal conductivity (<i>k</i> = 0.7 W/(m K) at 300 K), with “glass-like” behavior of thermal transport, atypical of the crystalline state, in combination with high fluoride ion electrical conductivity (σ<sub>dc</sub> = 0.012 S/m at 293 K) and relatively low activation enthalpy for electrical conduction (Δ<i>H</i><sub>σ</sub> = 0.378 ± 0.005 eV). The observed behavior of the thermal and electrical conductivities of the Pb<sub>1−<i>x</i></sub>Sc<sub><i>x</i></sub>F<sub>2+<i>x</i></sub> solid solution is due to structural disorder in the fluorine sublattice—which persists at room temperature—as a result of heterovalent substitutions of Sc<sup>3+</sup> for Pb<sup>2+</sup> cations. The thermal and electrical conductivities of single crystals of Pb<sub>1−<i>x</i></sub>Sc<sub><i>x</i></sub>F<sub>2+<i>x</i></sub> and Pb<sub>1−<i>x</i></sub>Cd<sub><i>x</i></sub>F<sub>2</sub> two-component solid solutions (CaF<sub>2</sub> structure) are compared to those of the β-PbF<sub>2</sub> (CaF<sub>2</sub> structure) and ScF<sub>3</sub> (ReO<sub>3</sub> structure) single-component fluorides.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 9","pages":"1117 - 1125"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645404","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701589
V. A. Nebol’sin, V. A. Yur’ev, A. S. Samofalova
This paper presents models of the hysteresis effects occurring on the wetting perimeter of a liquid-metal catalyst drop due to the effects caused on the contact angles by the edge of the end (tip) face of a nanowires (NW) and the linear tension of the three-phase contact interface. The contact angle hysteresis of the catalyst liquid drop on the end of an NW grown by the vapor → liquid → solid (VLS) scheme is due to its indifferent equilibrium at the wetting perimeter. The conclusion is drawn that the contact angle hysteresis in the catalyst drop wetting the NW crystal surface has a dual, not strictly equilibrium nature.
{"title":"Wetting Hysteresis Effects in Vapor → Liquid → Solid Growth of Nanowires","authors":"V. A. Nebol’sin, V. A. Yur’ev, A. S. Samofalova","doi":"10.1134/S0020168524701589","DOIUrl":"10.1134/S0020168524701589","url":null,"abstract":"<p>This paper presents models of the hysteresis effects occurring on the wetting perimeter of a liquid-metal catalyst drop due to the effects caused on the contact angles by the edge of the end (tip) face of a nanowires (NW) and the linear tension of the three-phase contact interface. The contact angle hysteresis of the catalyst liquid drop on the end of an NW grown by the vapor → liquid → solid (VLS) scheme is due to its indifferent equilibrium at the wetting perimeter. The conclusion is drawn that the contact angle hysteresis in the catalyst drop wetting the NW crystal surface has a dual, not strictly equilibrium nature.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 10","pages":"1272 - 1278"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645459","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168525700128
P. G. Ismailova, N. Z. Gasanov, A. A. Gajieva, K. M. Guseinova
We have grown single crystals of solid solutions based on the layered compound semiconductor TlGaS2 containing up to 2 mol % praseodymium and characterized them by X-ray diffraction. The optical absorption edge of the TlGaS2〈Pr〉 solid solutions has been studied in the temperature range 100–200 K, and the edge exciton peak position has been determined as a function of temperature for all of the TlGaS2〈Pr〉 compositions studied.
{"title":"Effect of Doping with Praseodymium on the Crystal Structure and Optical Absorption Edge of the TlGaS2 Compound","authors":"P. G. Ismailova, N. Z. Gasanov, A. A. Gajieva, K. M. Guseinova","doi":"10.1134/S0020168525700128","DOIUrl":"10.1134/S0020168525700128","url":null,"abstract":"<p>We have grown single crystals of solid solutions based on the layered compound semiconductor TlGaS<sub>2</sub> containing up to 2 mol % praseodymium and characterized them by X-ray diffraction. The optical absorption edge of the TlGaS<sub>2</sub>〈Pr〉 solid solutions has been studied in the temperature range 100–200 K, and the edge exciton peak position has been determined as a function of temperature for all of the TlGaS<sub>2</sub>〈Pr〉 compositions studied.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 11","pages":"1293 - 1298"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645398","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701607
D. M. Zimina, O. Yu. Troshin, A. Yu. Sozin
The vapor–liquid separation factors for the system Ni(PF3)4–impurities, in which the impurities include pentane (3.8 ± 0.8), hexane (1.3 ± 0.3), heptane (0.6 ± 0.2), dichloromethane (3.5 ± 0.8), trichloromethane (1.5 ± 0.3), tetrachloromethane (3.0 ± 0.7), phosphorus(III) fluoride (27.7.3 ± 7.8), and branched alkanes (2-methylpentane, 3-methylpentane, 2-methylhexane, 3-methylhexane, and 3-ethylhexane) were determined at 298 K by the static phase balancing method. The experimental data were in good agreement with the estimates of the vapor–liquid separation factors based on the conformal solution theory using Lennard-Jones potential parameters.
{"title":"Vapor–Liquid Equilibrium in the Ni(PF3)4–Hydrocarbon C5–C8 and Chloroalkane CH4–nCln (n = 2–4) System","authors":"D. M. Zimina, O. Yu. Troshin, A. Yu. Sozin","doi":"10.1134/S0020168524701607","DOIUrl":"10.1134/S0020168524701607","url":null,"abstract":"<p>The vapor–liquid separation factors for the system Ni(PF<sub>3</sub>)<sub>4</sub>–impurities, in which the impurities include pentane (3.8 ± 0.8), hexane (1.3 ± 0.3), heptane (0.6 ± 0.2), dichloromethane (3.5 ± 0.8), trichloromethane (1.5 ± 0.3), tetrachloromethane (3.0 ± 0.7), phosphorus(III) fluoride (27.7.3 ± 7.8), and branched alkanes (2-methylpentane, 3-methylpentane, 2-methylhexane, 3-methylhexane, and 3-ethylhexane) were determined at 298 K by the static phase balancing method. The experimental data were in good agreement with the estimates of the vapor–liquid separation factors based on the conformal solution theory using Lennard-Jones potential parameters.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 10","pages":"1279 - 1282"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645462","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701334
V. P. Smagin, P. M. Kotel’nikova
Composites based on poly(methylmethacrylate) (PMMA) and lead and europium salts, with the compositions PMMA/Pb(CF3COO)2 and PMMA/Pb(CF3COO)2,Eu(CF3COO)3, have been prepared by curing methylmethacrylate (MMA) based solutions via thermal radical block polymerization of MMA. The refractive index of MMA + Pb(CF3COO)2 solutions and the density of the PMMA/Pb(CF3COO)2 polymer composites have been shown to increase linearly as the Pb salt concentration increases to 83 wt % (40 wt % elemental Pb). The optical transmission of the composites at wavelengths above 450 nm and the highest lead and europium concentrations reaches 90% at sample thicknesses of up to 5 mm. The lead equivalent at a Pb(II) concentration of 40 wt % is 0.010. Photoluminescence in the PMMA/Pb(CF3COO)2,Eu(CF3COO)3 composites is due to Eu3+ electronic transitions from the 5D0 metastable electron energy level to the 7Fj sublevels of the ground level. We have demonstrated the influence of lead(II) and europium(III) on the properties of the matrix and the influence of the matrix and Pb(II) on absorption and luminescence spectra of europium(III).
{"title":"Europium-Containing Luminescent Composites Based on Lead(II)-Modified Poly(methylmethacrylate)","authors":"V. P. Smagin, P. M. Kotel’nikova","doi":"10.1134/S0020168524701334","DOIUrl":"10.1134/S0020168524701334","url":null,"abstract":"<p>Composites based on poly(methylmethacrylate) (PMMA) and lead and europium salts, with the compositions PMMA/Pb(CF<sub>3</sub>COO)<sub>2</sub> and PMMA/Pb(CF<sub>3</sub>COO)<sub>2</sub>,Eu(CF<sub>3</sub>COO)<sub>3</sub>, have been prepared by curing methylmethacrylate (MMA) based solutions via thermal radical block polymerization of MMA. The refractive index of MMA + Pb(CF<sub>3</sub>COO)<sub>2</sub> solutions and the density of the PMMA/Pb(CF<sub>3</sub>COO)<sub>2</sub> polymer composites have been shown to increase linearly as the Pb salt concentration increases to 83 wt % (40 wt % elemental Pb). The optical transmission of the composites at wavelengths above 450 nm and the highest lead and europium concentrations reaches 90% at sample thicknesses of up to 5 mm. The lead equivalent at a Pb(II) concentration of 40 wt % is 0.010. Photoluminescence in the PMMA/Pb(CF<sub>3</sub>COO)<sub>2</sub>,Eu(CF<sub>3</sub>COO)<sub>3</sub> composites is due to Eu<sup>3+</sup> electronic transitions from the <sup>5</sup><i>D</i><sub>0</sub> metastable electron energy level to the <sup>7</sup><i>F</i><sub><i>j</i></sub> sublevels of the ground level. We have demonstrated the influence of lead(II) and europium(III) on the properties of the matrix and the influence of the matrix and Pb(II) on absorption and luminescence spectra of europium(III).</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 9","pages":"1152 - 1160"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645463","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701528
K. B. Podbolotov, Yu. A. Egorova, L. V. Dogotar’, S. V. Vasilevich, A. N. Asadchii
Data on the thermochemical synthesis of molybdenum carbide on the basis of the (NH4)6Mo7O24–NH4NO3–C6H12N4 system at different component ratios have been reported. Thermodynamic computations have been performed to establish composition regions for probable exothermic reactions to produce molybdenum carbide: 10–20 moles of ammonium nitrate per 1 mole of ammonium molybdate and the ratio of reducing agent to oxidizing agent (φ) equal to 1.5–4.0. It has been found that the reaction in ammonium molybdate–ammonium nitrate–urotropin system includes several stages, the main exothermic reaction is observed after temperature of 120–180°C is reached. Molybdenum carbide forms at φ ≥ 6.5 after thermal treatment at 1000°C under inert atmosphere. The reaction leads to fine crystalline structure of particles with size of 100–200 nm. The obtained materials based on molybdenum carbide show catalytic activity in the conversion of products of incomplete combustion of biofuel (pyrolysis resins). Addition of the obtained materials to pyrolysis resin in 1/10 ratio enhances its conversion (rate parameter increases by 2–10 times), reduces average process temperature by 50–100°C, and decreases activation energy from 82 to 52–65 kJ/mol.
{"title":"Thermochemical Synthesis of Molybdenum Carbide on the Basis of the (NH4)6Mo7O24–NH4NO3–C6H12N4 System","authors":"K. B. Podbolotov, Yu. A. Egorova, L. V. Dogotar’, S. V. Vasilevich, A. N. Asadchii","doi":"10.1134/S0020168524701528","DOIUrl":"10.1134/S0020168524701528","url":null,"abstract":"<p>Data on the thermochemical synthesis of molybdenum carbide on the basis of the (NH<sub>4</sub>)<sub>6</sub>Mo<sub>7</sub>O<sub>24</sub>–NH<sub>4</sub>NO<sub>3</sub>–C<sub>6</sub>H<sub>12</sub>N<sub>4</sub> system at different component ratios have been reported. Thermodynamic computations have been performed to establish composition regions for probable exothermic reactions to produce molybdenum carbide: 10–20 moles of ammonium nitrate per 1 mole of ammonium molybdate and the ratio of reducing agent to oxidizing agent (φ) equal to 1.5–4.0. It has been found that the reaction in ammonium molybdate–ammonium nitrate–urotropin system includes several stages, the main exothermic reaction is observed after temperature of 120–180°C is reached. Molybdenum carbide forms at φ ≥ 6.5 after thermal treatment at 1000°C under inert atmosphere. The reaction leads to fine crystalline structure of particles with size of 100–200 nm. The obtained materials based on molybdenum carbide show catalytic activity in the conversion of products of incomplete combustion of biofuel (pyrolysis resins). Addition of the obtained materials to pyrolysis resin in 1/10 ratio enhances its conversion (rate parameter increases by 2–10 times), reduces average process temperature by 50–100°C, and decreases activation energy from 82 to 52–65 kJ/mol.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 10","pages":"1205 - 1215"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645485","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-18DOI: 10.1134/S0020168524701504
R. F. Al’mukhametov, A. D. Davletshina, V. V. Astanin, B. M. Akhmetgaliev
Abstract―Compound Cu3NaS2 has been prepared by solid-phase reactions from copper and sodium sulfides Cu2S and Na2S. It has been shown that compound Cu3NaS2 has hexagonal structure with lattice parameters a = 13.9398 ± 23 Å and c = 21.4637 ± 74 Å. After 6 months after synthesis, compound Cu3NaS2 spontaneously transforms at ambient temperature from hexagonal structure into phase with face-centered cubic (FCC) lattice. The dimension of coherent-scattering regions (CSR) for the FCC phase determined from the broadening of diffraction lines varies from ~25 nm at ambient temperature to ~110 nm at 500°C. DSC curves show anomalies at temperatures of 108 and 436°C corresponding to endothermal reversible transitions without change in the type of crystal lattice. The authors consider these anomalies to be due to redistribution of copper and sodium cations over possible crystallographic positions.
{"title":"Solid-Phase Synthesis and Structural Features of Compound Cu3NaS2","authors":"R. F. Al’mukhametov, A. D. Davletshina, V. V. Astanin, B. M. Akhmetgaliev","doi":"10.1134/S0020168524701504","DOIUrl":"10.1134/S0020168524701504","url":null,"abstract":"<p><b>Abstract</b>―Compound Cu<sub>3</sub>NaS<sub>2</sub> has been prepared by solid-phase reactions from copper and sodium sulfides Cu<sub>2</sub>S and Na<sub>2</sub>S. It has been shown that compound Cu<sub>3</sub>NaS<sub>2</sub> has hexagonal structure with lattice parameters <i>a</i> = 13.9398 ± 23 Å and <i>c</i> = 21.4637 ± 74 Å. After 6 months after synthesis, compound Cu<sub>3</sub>NaS<sub>2</sub> spontaneously transforms at ambient temperature from hexagonal structure into phase with face-centered cubic (FCC) lattice. The dimension of coherent-scattering regions (<b>CSR</b>) for the FCC phase determined from the broadening of diffraction lines varies from ~25 nm at ambient temperature to ~110 nm at 500°C. DSC curves show anomalies at temperatures of 108 and 436°C corresponding to endothermal reversible transitions without change in the type of crystal lattice. The authors consider these anomalies to be due to redistribution of copper and sodium cations over possible crystallographic positions.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 10","pages":"1172 - 1179"},"PeriodicalIF":0.9,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143645481","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-13DOI: 10.1134/S0020168524701322
T. M. Zima, N. F. Uvarov
One-dimensional layered α-МоО3 structures have been synthesized via hydrothermal treatment of peroxo molybdenum complexes. Treatment of the structures in aqueous sucrose solutions under hydrothermal conditions after drying at 80°C has been shown to cause partial reduction of their surface. The reduction process is accompanied by a change in Mo–O bond length as a consequence of distortion of the MoO6 octahedra. Local supersaturation with reduction products in aqueous solution under hydrothermal conditions leads to the formation of new crystallization centers and growth of dumbbell-shaped particles. The forming nanostructured α-МоО3/MoO2 two-phase material, with two morphological species of particles, contains no carbon. Such a strategy for designing one-dimensional α-МоО3 structures can be aimed at monitoring electrochemical degradation of high-capacity electrodes and controlling the associated deformation dynamics.
{"title":"Synthesis of One-Dimensional Molybdenum Trioxide Structures and Influence of Aqueous Sucrose Solution on Hydrothermal Treatment of the Structures","authors":"T. M. Zima, N. F. Uvarov","doi":"10.1134/S0020168524701322","DOIUrl":"10.1134/S0020168524701322","url":null,"abstract":"<p>One-dimensional layered α-МоО<sub>3</sub> structures have been synthesized via hydrothermal treatment of peroxo molybdenum complexes. Treatment of the structures in aqueous sucrose solutions under hydrothermal conditions after drying at 80°C has been shown to cause partial reduction of their surface. The reduction process is accompanied by a change in Mo–O bond length as a consequence of distortion of the MoO<sub>6</sub> octahedra. Local supersaturation with reduction products in aqueous solution under hydrothermal conditions leads to the formation of new crystallization centers and growth of dumbbell-shaped particles. The forming nanostructured α-МоО<sub>3</sub>/MoO<sub>2</sub> two-phase material, with two morphological species of particles, contains no carbon. Such a strategy for designing one-dimensional α-МоО<sub>3</sub> structures can be aimed at monitoring electrochemical degradation of high-capacity electrodes and controlling the associated deformation dynamics.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 8","pages":"976 - 982"},"PeriodicalIF":0.9,"publicationDate":"2025-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143602337","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-03-13DOI: 10.1134/S0020168524701267
Yu. V. Bogatov, V. A. Shcherbakov, D. Yu. Kovalev, N. P. Cherezov, T. V. Barinova, O. D. Boyarchenko, M. I. Alymov
Titanium nickelide alloys have been prepared by self-propagating high-temperature synthesis compaction using equiatomic mixtures of nickel and titanium powders. The alloys were synthesized in a “sand” press die with the use of a “chemical furnace” and in a rigid press die. In the latter process, reaction mixtures were first subjected to mechanical activation (MA), which made it possible to carry out exothermic synthesis and consolidation of the synthesis products without preheating. No inert atmosphere was used in the syntheses. We obtained titanium nickelide samples 70 mm in diameter and 8 mm in thickness. The percentage of the NiTi phase has been shown to depend on the combustion temperature of the Ni + Ti powder mixture and the percentages of oxygen and hydrogen in the starting titanium powder. The largest percentage of the NiTi phase (85 vol %) was reached at a combustion temperature of 1400°C with the use of titanium containing 0.55 wt % oxygen and 0.14 wt % hydrogen. An increase in the oxygen content of the Ni + Ti powder mixture to 2.3 wt % as a result of MA leads to an increase in the content of the Ti2Ni phase in the alloy to 53 vol %. As the hydrogen content of titanium increases to 0.6 wt %, the combustion temperature and speed decrease and free Ni remains in the alloy. The alloys with the highest content of the NiTi phase have the lowest microhardness: HV = 6.2 GPa. As the percentage of the Ti2Ni, Ni3Ti, and Ni4Ti3 phases in the alloys increases, their hardness rises to HV = 11.1 GPa.
{"title":"Self-Propagating High-Temperature Synthesis Compaction of Titanium Nickelide: Effect of Oxygen and Hydrogen Impurities on the Structure and Properties of the Alloys","authors":"Yu. V. Bogatov, V. A. Shcherbakov, D. Yu. Kovalev, N. P. Cherezov, T. V. Barinova, O. D. Boyarchenko, M. I. Alymov","doi":"10.1134/S0020168524701267","DOIUrl":"10.1134/S0020168524701267","url":null,"abstract":"<p>Titanium nickelide alloys have been prepared by self-propagating high-temperature synthesis compaction using equiatomic mixtures of nickel and titanium powders. The alloys were synthesized in a “sand” press die with the use of a “chemical furnace” and in a rigid press die. In the latter process, reaction mixtures were first subjected to mechanical activation (MA), which made it possible to carry out exothermic synthesis and consolidation of the synthesis products without preheating. No inert atmosphere was used in the syntheses. We obtained titanium nickelide samples 70 mm in diameter and 8 mm in thickness. The percentage of the NiTi phase has been shown to depend on the combustion temperature of the Ni + Ti powder mixture and the percentages of oxygen and hydrogen in the starting titanium powder. The largest percentage of the NiTi phase (85 vol %) was reached at a combustion temperature of 1400°C with the use of titanium containing 0.55 wt % oxygen and 0.14 wt % hydrogen. An increase in the oxygen content of the Ni + Ti powder mixture to 2.3 wt % as a result of MA leads to an increase in the content of the Ti<sub>2</sub>Ni phase in the alloy to 53 vol %. As the hydrogen content of titanium increases to 0.6 wt %, the combustion temperature and speed decrease and free Ni remains in the alloy. The alloys with the highest content of the NiTi phase have the lowest microhardness: <i>HV</i> = 6.2 GPa. As the percentage of the Ti<sub>2</sub>Ni, Ni<sub>3</sub>Ti, and Ni<sub>4</sub>Ti<sub>3</sub> phases in the alloys increases, their hardness rises to <i>HV</i> = 11.1 GPa.</p>","PeriodicalId":585,"journal":{"name":"Inorganic Materials","volume":"60 8","pages":"960 - 969"},"PeriodicalIF":0.9,"publicationDate":"2025-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143602121","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}