Pub Date : 2026-02-19DOI: 10.1134/S2075113325702569
M. A. Babuev, V. V. Ovchinnikov
The influence of a thin-film copper coating deposited by magnetron sputtering on a sample of the VT6 titanium alloy is studied at the running-in stage in a friction pair of the VT6 titanium alloy and ShKh-15 steel. The results are compared with a sample of the VT6 titanium alloy without a copper film. The composition of a thin copper film is studied by elements before and after wear testing using scanning electron microscopy. It is established that the VT6 alloy sample with deposited copper coating is characterized by a shorter running-in time and mass wear.
{"title":"Magnetron Sputtering of Thin Copper Films to Increase Wear Resistance of Titanium Alloy VT6","authors":"M. A. Babuev, V. V. Ovchinnikov","doi":"10.1134/S2075113325702569","DOIUrl":"10.1134/S2075113325702569","url":null,"abstract":"<p>The influence of a thin-film copper coating deposited by magnetron sputtering on a sample of the VT6 titanium alloy is studied at the running-in stage in a friction pair of the VT6 titanium alloy and ShKh-15 steel. The results are compared with a sample of the VT6 titanium alloy without a copper film. The composition of a thin copper film is studied by elements before and after wear testing using scanning electron microscopy. It is established that the VT6 alloy sample with deposited copper coating is characterized by a shorter running-in time and mass wear.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"17 1","pages":"148 - 153"},"PeriodicalIF":0.3,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147339965","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-19DOI: 10.1134/S2075113325702661
A. M. Drits, V. V. Ovchinnikov, R. B. Reztsov
The results of experimental studies are given on the effect of the welding method of butt joints made in sheets of alloy 1565ch. The level and distribution of transverse residual stresses are investigated. It is proved that, depending on technique, fusion welding results in tensile stresses of 65–120 MPa developing in the central region of the weld. The residual compression stresses of 8–15 MPa are observed in the weld zone during friction stir welding. Annealing of welded joints at 280–300°C for 30 min completely relaxes the residual stress. The application of electrodynamic processing with an exposure time of 0.7–1.8 ms lifts the tensile stresses in the welded joints of alloy 1565chM obtained through fusion welding and forms a stable zone of compression stresses in the mixing zone of joints obtained using friction stir welding.
{"title":"Effect of Welding Method on Residual Stresses in Welded Joints Made of Aluminum Alloy 1565ch","authors":"A. M. Drits, V. V. Ovchinnikov, R. B. Reztsov","doi":"10.1134/S2075113325702661","DOIUrl":"10.1134/S2075113325702661","url":null,"abstract":"<p>The results of experimental studies are given on the effect of the welding method of butt joints made in sheets of alloy 1565ch. The level and distribution of transverse residual stresses are investigated. It is proved that, depending on technique, fusion welding results in tensile stresses of 65–120 MPa developing in the central region of the weld. The residual compression stresses of 8–15 MPa are observed in the weld zone during friction stir welding. Annealing of welded joints at 280–300°C for 30 min completely relaxes the residual stress. The application of electrodynamic processing with an exposure time of 0.7–1.8 ms lifts the tensile stresses in the welded joints of alloy 1565chM obtained through fusion welding and forms a stable zone of compression stresses in the mixing zone of joints obtained using friction stir welding.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"17 1","pages":"222 - 228"},"PeriodicalIF":0.3,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147340474","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-19DOI: 10.1134/S2075113325702582
Kh. V. Allahverdiyeva, N. T. Kakhramanov
This paper presents the results of a study examining the effects of mechanical activation of graphite nanoparticles and heat treatment of nanocomposites on their key physicomechanical and physicochemical properties. Polyolefins such as ethylene/hexene copolymer, ethylene/butene copolymer, ethylene/propylene random copolymer, and ethylene/propylene block copolymer have been used. The objective of the study was to explore the feasibility of producing multifunctional nanocomposites based on these materials that exhibit electrical conductivity, wear resistance, strength, and satisfactory melt flowability for processing by injection molding and extrusion methods.
{"title":"Influence of Mechanoactivation of Graphite Nanoparticles on Electrical Conductivity and Physical and Mechanical Properties of Multifunctional Nanocomposites Based on Copolymers of Ethylene with α-Olefins","authors":"Kh. V. Allahverdiyeva, N. T. Kakhramanov","doi":"10.1134/S2075113325702582","DOIUrl":"10.1134/S2075113325702582","url":null,"abstract":"<p>This paper presents the results of a study examining the effects of mechanical activation of graphite nanoparticles and heat treatment of nanocomposites on their key physicomechanical and physicochemical properties. Polyolefins such as ethylene/hexene copolymer, ethylene/butene copolymer, ethylene/propylene random copolymer, and ethylene/propylene block copolymer have been used. The objective of the study was to explore the feasibility of producing multifunctional nanocomposites based on these materials that exhibit electrical conductivity, wear resistance, strength, and satisfactory melt flowability for processing by injection molding and extrusion methods.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"17 1","pages":"161 - 168"},"PeriodicalIF":0.3,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147340501","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-19DOI: 10.1134/S2075113325702405
A. A. Shmatov, L. Soos, Z. Krajny
Scientific principles of hydrochemical dispersion of inorganic nonmetal powder materials are formulated. The effect of hydrochemical nanodispersion of quartz and chalk microparticles under the conditions of a wedging destructive action of surface-active substances and a “pseudocavitation” thermohydrodynamic action of a boiling suspension upon a fast-repeating interchange of thermal, chemical, and physical gradients generated in a coarsely dispersed system is found. A geometric model of the origination of this process is developed, and a generalized equation describing the effect of various processing parameters on the degree of hydrochemical dispersion of inorganic ceramic-forming particles is proposed. The following is determined on the basis of the investigation of the effect of hydrochemical treatment on the change in the sizes and volume fraction of dispersed quartz and chalk particles in an aqueous dispersion medium: (1) two opposite processes compete in the process of hydrochemical treatment, namely, nanodispersion and aggregation of nanoparticles, and (2) upon long-term execution of hydrochemical treatment, the aggregates obtained in an aqueous dispersion medium are broken down to nanoobjects, increasing the fraction of nanoparticles in the dispersed system.
{"title":"Realization of Effect of Hydrochemical Dispersion of Materials","authors":"A. A. Shmatov, L. Soos, Z. Krajny","doi":"10.1134/S2075113325702405","DOIUrl":"10.1134/S2075113325702405","url":null,"abstract":"<p>Scientific principles of hydrochemical dispersion of inorganic nonmetal powder materials are formulated. The effect of hydrochemical nanodispersion of quartz and chalk microparticles under the conditions of a wedging destructive action of surface-active substances and a “pseudocavitation” thermohydrodynamic action of a boiling suspension upon a fast-repeating interchange of thermal, chemical, and physical gradients generated in a coarsely dispersed system is found. A geometric model of the origination of this process is developed, and a generalized equation describing the effect of various processing parameters on the degree of hydrochemical dispersion of inorganic ceramic-forming particles is proposed. The following is determined on the basis of the investigation of the effect of hydrochemical treatment on the change in the sizes and volume fraction of dispersed quartz and chalk particles in an aqueous dispersion medium: (1) two opposite processes compete in the process of hydrochemical treatment, namely, nanodispersion and aggregation of nanoparticles, and (2) upon long-term execution of hydrochemical treatment, the aggregates obtained in an aqueous dispersion medium are broken down to nanoobjects, increasing the fraction of nanoparticles in the dispersed system.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"17 1","pages":"35 - 40"},"PeriodicalIF":0.3,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147340510","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-19DOI: 10.1134/S2075113325702417
E. L. Kolyvanov, V. P. Korzhov
Temperature dependences of shear modulus and internal friction are studied in the range from 130 to 600 K for Cu–Ni, Ti–Ti5Si3, and EP678–Me3Al metal laminate samples. In the initial state of samples, at temperatures below room temperature, a peak in internal friction and a stepwise change in the shear modulus are observed. After high-temperature annealing, these features disappear. Possible mechanisms for this observed behavior are discussed.
{"title":"Shear Modulus and Internal Friction in Multilayer Metal Composites","authors":"E. L. Kolyvanov, V. P. Korzhov","doi":"10.1134/S2075113325702417","DOIUrl":"10.1134/S2075113325702417","url":null,"abstract":"<p>Temperature dependences of shear modulus and internal friction are studied in the range from 130 to 600 K for Cu–Ni, Ti–Ti<sub>5</sub>Si<sub>3</sub>, and EP678–Me<sub>3</sub>Al metal laminate samples. In the initial state of samples, at temperatures below room temperature, a peak in internal friction and a stepwise change in the shear modulus are observed. After high-temperature annealing, these features disappear. Possible mechanisms for this observed behavior are discussed.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"17 1","pages":"41 - 47"},"PeriodicalIF":0.3,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147340511","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-08DOI: 10.1134/S2075113325701965
M. G. Ostapenko, V. O. Semin, S. I. Yuzhakova, F. A. D’yachenko, K. P. Savkin
The detailed comparative XRD, TEM/EDS analysis of TiNi and TiNiCuZr samples revealed the formation of two isostructural B2 phases with different lattice parameters, chemical composition and microstructure. According to the experimental the lattice parameter value aB2(TiNiCuZr) in the TiNiCuZr sample is several times higher than aB2(TiNi) in the TiNi sample, indicating the formation of a new B2 phase. These variations in B2 lattice parameters strongly correlate with the changes in the chemical composition. The study of the electrochemical properties of the initial alloys (TiNi, Ti–Ni–Cu–Zr) in 0.9 wt % NaCl and artificial saliva showed that the TiNi alloy of binary composition exhibits significantly higher corrosion properties. In turn, the Ti–Ni–Cu–Zr alloy is prone to anodic polarization and corrosion destruction. It was found that under the same conditions of the corrosive media, the corrosion rate of the Ti–Ni–Cu–Zr alloy is ∼3.2 times higher than that of the TiNi alloys.
{"title":"Effect of Zr and Cu Alloying on the Structure and Electrochemical Properties of TiNi","authors":"M. G. Ostapenko, V. O. Semin, S. I. Yuzhakova, F. A. D’yachenko, K. P. Savkin","doi":"10.1134/S2075113325701965","DOIUrl":"10.1134/S2075113325701965","url":null,"abstract":"<p>The detailed comparative XRD, TEM/EDS analysis of TiNi and TiNiCuZr samples revealed the formation of two isostructural B2 phases with different lattice parameters, chemical composition and microstructure. According to the experimental the lattice parameter value <i>a</i><sub>B2</sub>(TiNiCuZr) in the TiNiCuZr sample is several times higher than <i>a</i><sub>B2</sub>(TiNi) in the TiNi sample, indicating the formation of a new B2 phase. These variations in B2 lattice parameters strongly correlate with the changes in the chemical composition. The study of the electrochemical properties of the initial alloys (TiNi, Ti–Ni–Cu–Zr) in 0.9 wt % NaCl and artificial saliva showed that the TiNi alloy of binary composition exhibits significantly higher corrosion properties. In turn, the Ti–Ni–Cu–Zr alloy is prone to anodic polarization and corrosion destruction. It was found that under the same conditions of the corrosive media, the corrosion rate of the Ti–Ni–Cu–Zr alloy is ∼3.2 times higher than that of the TiNi alloys.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"16 6","pages":"1743 - 1751"},"PeriodicalIF":0.3,"publicationDate":"2025-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698376","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-08DOI: 10.1134/S2075113325702247
V. A. Bykov, D. A. Yagodin, T. V. Kulikova, S. Kh. Estemirova
The development of new functional and structural materials constitutes one of the priority areas of modern materials science. Accurate knowledge of the thermal properties of systems under study is important for obtaining new effective multifunctional materials with high practical performance. In this paper, we investigate the effect of the composition of the Ni–Zr system on important thermophysical properties such as heat capacity, thermal expansion coefficient (CTE), and thermal conductivity. The temperature dependences of the thermophysical properties of polycrystalline Ni–Zr samples are considered, and the influence of structure effects on their behavior is discussed. The phase compositions of the alloys were confirmed by X-ray structural analysis. The deviation of density from the additive value reaches 5% and has a pronounced minimum at 50 at % Ni. The CTE curves of the annealed samples show two extremes at nickel concentrations of 77 and 50 at %. Deviations in the CTE values on the concentration curve are typical for samples with concentrations close to the formation of NiZr2 and NiZr intermetallics. The temperature curves of the thermal diffusivity and thermal conductivity of Ni–Zr alloys are non-monotonically. The defective structure of polycrystalline Ni–Zr samples has a noticeable effect on their thermophysical properties.
新型功能材料和结构材料的开发是现代材料科学的重点领域之一。准确了解所研究体系的热性能对于获得具有高实用性能的新型有效多功能材料具有重要意义。在本文中,我们研究了Ni-Zr体系的组成对热容、热膨胀系数(CTE)和导热系数等重要热物理性能的影响。研究了Ni-Zr多晶样品热物理性能的温度依赖性,并讨论了结构效应对其性能的影响。通过x射线结构分析确定了合金的相组成。密度与添加剂值的偏差达到5%,在50% at % Ni时有明显的最小值。退火后样品的CTE曲线在镍浓度为77%和50%时呈现两个极端。对于浓度接近NiZr2和NiZr金属间化合物形成的样品,CTE值在浓度曲线上的偏差是典型的。Ni-Zr合金的热扩散率和热导率的温度曲线是非单调的。Ni-Zr多晶样品的缺陷结构对其热物理性能有显著影响。
{"title":"Polycrystalline Ni–Zr Alloys: Thermal Expansion, Density, Thermal Diffusivity and Thermal Conductivity","authors":"V. A. Bykov, D. A. Yagodin, T. V. Kulikova, S. Kh. Estemirova","doi":"10.1134/S2075113325702247","DOIUrl":"10.1134/S2075113325702247","url":null,"abstract":"<p>The development of new functional and structural materials constitutes one of the priority areas of modern materials science. Accurate knowledge of the thermal properties of systems under study is important for obtaining new effective multifunctional materials with high practical performance. In this paper, we investigate the effect of the composition of the Ni–Zr system on important thermophysical properties such as heat capacity, thermal expansion coefficient (CTE), and thermal conductivity. The temperature dependences of the thermophysical properties of polycrystalline Ni–Zr samples are considered, and the influence of structure effects on their behavior is discussed. The phase compositions of the alloys were confirmed by X-ray structural analysis. The deviation of density from the additive value reaches 5% and has a pronounced minimum at 50 at % Ni. The CTE curves of the annealed samples show two extremes at nickel concentrations of 77 and 50 at %. Deviations in the CTE values on the concentration curve are typical for samples with concentrations close to the formation of NiZr<sub>2</sub> and NiZr intermetallics. The temperature curves of the thermal diffusivity and thermal conductivity of Ni–Zr alloys are non-monotonically. The defective structure of polycrystalline Ni–Zr samples has a noticeable effect on their thermophysical properties.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"16 6","pages":"1935 - 1944"},"PeriodicalIF":0.3,"publicationDate":"2025-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698475","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-08DOI: 10.1134/S2075113325701795
N. M. Barbin, S. A. Titiov
The article presents the results of thermodynamic modeling of the behavior of Am, Pu, Cs radionuclides when radioactive graphite is heated with an atmospheric atmosphere. Using the TERRA software package, thermodynamic analysis was performed in the temperature range from 300 to 3600 K in order to determine the possible composition of the ionized, gaseous and condensed phases. It has been established that americium in the temperature range from 300 to 2200 K is in the form of condensed AmO2(k). When the temperature rises from 2200 to 3600 K, it is in the form of gaseous Am and condensed Am2O3(k). Plutonium in the range of temperatures from 700 to 1200 K is in the form of condensed PuCl3(k), PuOCl(k) with an increase in temperature from 1900 to 3600 K in the form of gaseous PuO2, PuO in the form of condensed PuO2(k), Pu2O3(k) and ionized PuO+. Caesium at temperatures from 600 to 900 K is in the form of condensed CsCl(k) and gaseous CsCl as the temperature rises from 1300 to 1700 K in the form of ionized PuO+. The main reactions within individual phases and between condensed, gaseous and ionized phases are determined in this work. Calculations of the equilibrium constants of their reactions have been carried out.
{"title":"Thermodynamic Modeling of the Behavior of Am, Pu, Cs Radionuclides during Heating of Reactor Graphite in an Air Atmosphere","authors":"N. M. Barbin, S. A. Titiov","doi":"10.1134/S2075113325701795","DOIUrl":"10.1134/S2075113325701795","url":null,"abstract":"<p>The article presents the results of thermodynamic modeling of the behavior of Am, Pu, Cs radionuclides when radioactive graphite is heated with an atmospheric atmosphere. Using the TERRA software package, thermodynamic analysis was performed in the temperature range from 300 to 3600 K in order to determine the possible composition of the ionized, gaseous and condensed phases. It has been established that americium in the temperature range from 300 to 2200 K is in the form of condensed AmO<sub>2(k)</sub>. When the temperature rises from 2200 to 3600 K, it is in the form of gaseous Am and condensed Am<sub>2</sub>O<sub>3(k)</sub>. Plutonium in the range of temperatures from 700 to 1200 K is in the form of condensed PuCl<sub>3(k)</sub>, PuOCl<sub>(k)</sub> with an increase in temperature from 1900 to 3600 K in the form of gaseous PuO<sub>2</sub>, PuO in the form of condensed PuO<sub>2(k)</sub>, Pu<sub>2</sub>O<sub>3(k)</sub> and ionized PuO<sup>+</sup>. Caesium at temperatures from 600 to 900 K is in the form of condensed CsCl<sub>(k)</sub> and gaseous CsCl as the temperature rises from 1300 to 1700 K in the form of ionized PuO<sup>+</sup>. The main reactions within individual phases and between condensed, gaseous and ionized phases are determined in this work. Calculations of the equilibrium constants of their reactions have been carried out.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"16 6","pages":"1631 - 1634"},"PeriodicalIF":0.3,"publicationDate":"2025-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698514","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-08DOI: 10.1134/S2075113325702168
N. V. Zemlyakova, S. O. Rogachev
In this work, the methods of scanning electron microscopy and transmission electron microscopy to study the deformation refinement of copper grains from 200 μm to 50 nm in a 20 mm workpiece’s cross section were used. A grain refinement pattern during the transition of the copper structure from mesolevel (d ≥ 250 nm) to the microlevel (d < 250 nm) after drawing and two, six, and eight passes of the ECAP along the Вс route at room temperature was proposed. It was shown that when shear bands intersect at an angle of 45°, grains in the form of rhombuses or hexagons with a width of 500–800 nm are separated by subgrains with a width of 150–250 nm with their own structure of nano bands with a width of 50 nm, and submicrograins of 50–100 nm. After 8 passes ECAP, high-angle grain boundaries of hexagons were formed at the location of triple grain junctions as a result of primary recrystallization. The scheme of deformation grain refinement was changed as follows. After two ECAP passes, microbands with a cellular structure 100–200 nm wide with an apex angle of 45° were formed. This herringbone-like shear bands were formed. After six ECAP passes, a banded and “lattice” structure was formed at the places of multiple intersections of shear bands, with rhombohedrons forming in the center. After eight ECAP passes, the resulting grain refinement pattern consisted of fragmented shear bands of 400–500 nm wide and shear bands of 300 nm wide located at an angle of 45°.
{"title":"Formation of Rhombohedrons in the Copper Structure after Drawing and Equal Channel Angular Pressing","authors":"N. V. Zemlyakova, S. O. Rogachev","doi":"10.1134/S2075113325702168","DOIUrl":"10.1134/S2075113325702168","url":null,"abstract":"<p>In this work, the methods of scanning electron microscopy and transmission electron microscopy to study the deformation refinement of copper grains from 200 μm to 50 nm in a 20 mm workpiece’s cross section were used. A grain refinement pattern during the transition of the copper structure from mesolevel (<i>d</i> ≥ 250 nm) to the microlevel (<i>d</i> < 250 nm) after drawing and two, six, and eight passes of the ECAP along the Вс route at room temperature was proposed. It was shown that when shear bands intersect at an angle of 45°, grains in the form of rhombuses or hexagons with a width of 500–800 nm are separated by subgrains with a width of 150–250 nm with their own structure of nano bands with a width of 50 nm, and submicrograins of 50–100 nm. After 8 passes ECAP, high-angle grain boundaries of hexagons were formed at the location of triple grain junctions as a result of primary recrystallization. The scheme of deformation grain refinement was changed as follows. After two ECAP passes, microbands with a cellular structure 100–200 nm wide with an apex angle of 45° were formed. This herringbone-like shear bands were formed. After six ECAP passes, a banded and “lattice” structure was formed at the places of multiple intersections of shear bands, with rhombohedrons forming in the center. After eight ECAP passes, the resulting grain refinement pattern consisted of fragmented shear bands of 400–500 nm wide and shear bands of 300 nm wide located at an angle of 45°.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"16 6","pages":"1883 - 1888"},"PeriodicalIF":0.3,"publicationDate":"2025-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698674","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-08DOI: 10.1134/S2075113325702211
O. D. Pashkov, D. V. Kharitonov, D. A. Mikhalevsky, K. V. Pechenkin
This study demonstrates the results of incorporating granulated filler into quartz glass-based slurry to intensify the forming process. The use of porous granules reduces ceramic product forming time by more than half. The introduced granules serve a reinforcing function while improving workpiece density uniformity, minimizing slurry stratification rial properties were investigated and compared with those obtained via alternative manufacturing technologies.
{"title":"Quartz Ceramics Produced by Slip Casting with Granules","authors":"O. D. Pashkov, D. V. Kharitonov, D. A. Mikhalevsky, K. V. Pechenkin","doi":"10.1134/S2075113325702211","DOIUrl":"10.1134/S2075113325702211","url":null,"abstract":"<p>This study demonstrates the results of incorporating granulated filler into quartz glass-based slurry to intensify the forming process. The use of porous granules reduces ceramic product forming time by more than half. The introduced granules serve a reinforcing function while improving workpiece density uniformity, minimizing slurry stratification rial properties were investigated and compared with those obtained via alternative manufacturing technologies.</p>","PeriodicalId":586,"journal":{"name":"Inorganic Materials: Applied Research","volume":"16 6","pages":"1918 - 1921"},"PeriodicalIF":0.3,"publicationDate":"2025-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145698677","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}