Mechanical properties of chromium-manganese austenite steels in a hydrogen environment

We study the influence of gaseous hydrogen on the mechanical properties of hardened and deformed specimens of 07Kh13G20AN4 and 03Kh13N9G19AM2 steels under a pressure of 35 MPa in the temperature range 293–773 K. We establish that hydrogen causes the strain martensite transformation of nitrogen-containing austenite stable in air. Formation of a polygonal dislocation substructure by means of preliminary mechanical or thermomechanical treatment significantly decreases the tendency of steels toward hydrogen degradation. Karpenko Physicomechanical Institute, Ukrainian Academy of Sciences, L'viv. Translated from Fizyko-Khimichna Mekhanika Materialiv, Vol. 35, No. 5, pp. 75–78, September–October, 1999.     

Effect of prior austenite on reversed austenite stability and mechanical properties of low carbon medium manganese steel heavy plate

The effect of prior austenite on reversed austenite stability and mechanical properties of Fe‐0.06C‐0.2Si‐5.5Mn‐0.4Cr (wt.%) annealed steels was elucidated. With the decrease of austenitizing temperature from 1250 °C to 980 °C, the prior austenite changed from complete recrystallization to partial recrystallization, and the average austenite size was reduced. The volume fraction of reversed austenite was increased from 26.32 % to 30.25 % because of high density of grain boundaries and dislocations. The martensite transformation temperature of annealed steels was increased from ～115 °C to ～150 °C, and both of thermal and mechanical stability of reversed were reduced. There was no significant different in tensile properties, however, the impact toughness was enhanced from 100 J to 180 J at ?60 °C. The excellent impact toughness in annealed steel (austenitized at 980 °C) was obtained because of higher density of high misorientation grain boundaries, more volume fraction of reversed austenite and reduced segregation at grain boundaries.     

Mechanical stability of retained austenite during plastic deformation of super high strength carbide free bainitic steels

New carbide free bainitic microstructures are gaining an increasing interest on behalf the scientific and industrial community. The excellent combination of mechanical properties achieved in those microstructures with no need of complex heat treatments or thermomechanical processes represents their main advantage. The strength is mainly achieved by means of the very fine bainitic ferrite plates, consequence of the transformation mechanism, but the parameters contributing to the ductility of those microstructures are still unclear in this type of microstructures, where a soft phase, retained austenite, is imbibed in a very strong matrix of bainitic ferrite. A priori is reasonable to assume that retained austenite will control the levels of ductility achieved. Further enhancement of ductility can be achieved by the transformation of retained austenite into martensite (strain or stress assisted), thus its mechanical stability plays an important role in the final ductility. In this study, by means of X-ray analysis of interrupted compression tests, it is studied the influence that different microstructural aspects of retained austenite may have on its mechanical stability.     

Mechanical and magnetic properties of nickel-dispersed tetragonal zirconia nanocomposites

Effects of Ni dispersions on microstructure and mechanical properties have been studied for Y2O3-stabilized tetragonal zirconia (Y-TZP)/Ni nanocomposites with Ni dispersion up to 10 vol%. Composites were successfully fabricated by reducing and hot-pressing Y-TZP/NiO powder mixtures. Fracture strength was significantly improved from 1.5 GPa for monolithic Y-TZP to 1.9 GPa for nanocomposites with a small addition of Ni (1-2 vol%). Magnetic properties of Y-TZP/Ni nanocomposites were also investigated. Magnetization curves of Y-TZP/Ni nanocomposites showed typical hysteresis loops of soft magnetic materials, whereas coercivity was much larger than that of pure Ni metal. A new function arising from magnetomechanical effects of metallic Ni is also discussed for the present nanocomposites.     

Tuning austenite stability in a medium Mn steel and relationship to structure and mechanical properties

We study here the underlying factors that govern the stability of austenite in a medium Mn (Fe–0.18C–11Mn–3.8Al) (wt-%) steel. In this regard, a novel heat treatment involving intercritical quenching and tempering was designed to obtain high total elongation (TEL) and high ultimate tensile strength (UTS) in the cold-rolled steel. And the UTS and TEL approached 920–1150?MPa and 35–65%, respectively. The product of TEL and UTS (PSE) exceeded 40?GPa%, with a maximum value of 60?GPa%. A detailed analysis of microstructure before and after tensile deformation revealed that the TRIP effect occurred and the stability of austenite was predominantly governed by the grain sizes of austenite rather than the orientation of austenite grains. The theoretical analysis of work hardening data suggested that the superior elongation of medium Mn TRIP steel is related to the high stability of austenite and the cooperative deformation of ferrite.     

Mechanical properties and thermal stability of nitrogen incorporated diamond-like carbon films

The nitrogen incorporated diamond-like carbon films were deposited on Si (100) substrates by arc ion plating (AIP) under different N₂ content in the gas mixture of Ar and N₂. The influence of N₂ content on the film microstructure and mechanical properties was studied by atomic force microscopy, transmission electron microscopy, Raman spectroscopy, X-ray photoelectron spectroscopy (XPS) and nanoindentation. It was found that the hardness (H), elastic modulus (E), elastic recovery (R) and plastic resistance parameter (H/E) decrease with increasing the nitrogen content. The decrease of mechanical properties of DLC films resulted from nitrogen incorporation was associated with total sp³ carbon bond content and N-sp³C bond content. The structural modification as well as mechanical properties of the annealed nitrogen incorporated diamond-like carbon films was investigated as a function of annealing temperature. Raman spectra indicate that the I_D/I_G ratio starts to increase and G peak position shifts upward at the annealing temperature over 500 °C. The hardness and elastic modulus of thermally annealed nitrogen incorporated DLC films decreased slightly at lower annealing temperature and then significantly decreased at higher annealing temperature. The strong covalent bonding between C and N atoms is expected to be effective on their thermal stability enhancement.     

Mechanical and magnetic properties of the rapidly quenched Cu2MnAl

Rapidly solidified Cu₂MnAl ribbons were fabricated by the chill-block melt-spinning technique as a function of rotation speed of an iron roller. The rapidly quenched ribbons were relatively ductile, and the total strain at failure for the bend test increased with increasing rotation speed of the roller. The effect of rapid quenching on long-range ordering in Cu₂MnAl alloy was studied by X-ray diffraction. The decomposition characteristics during isothermal ageing at temperatures between 350 and 600° C were also examined by X-ray diffraction, magnetization and Vickers hardness measurements. The decomposition reaction at temperatures below 400° C was Cu₂MnAl-Cu₉Al₄+T-Cu₃Mn₂Al+-Mn. However, at temperatures between 500 and 600° C, Cu₂MnAl decomposed into a new L2₁ type Cu₂MnAl and-Mn, and further annealing caused the appearance of-Cu₉Al₄. The decomposition rate of the rapidly quenched ribbons was faster than that of the water-quenched alloy.     

Electronic and magnetic properties and structural stability of BeO sheet and nanoribbons

The novel electronic and magnetic properties of BeO nanoribbons (BeO NRs) as well as their stability are investigated through extensive density functional theory calculations. Different from semiconducting graphene nanoribbons and insulating BN ribbons, all zigzag edged BeO NRs are revealed to display ferromagnetic and metallic natures independent of the ribbon width and edge passivation. The polarized electron spins in H-passivated zigzag BeO NRs are from the unpaired electrons around the weakly formed Be-H bonds, while those of bare zigzag BeO NRs are due to the 2p states of edge O atoms. In sharp contrast, all armchair BeO NRs are nonmagnetic insulators regardless of the edge passivation. In particular, all bare armchair BeO NRs have a nearly constant band gap due to a peculiar edge localization effect. Interestingly, the band gaps of all armchair BeO NRs can be markedly reduced by an applied transverse electric field and even completely closed at a critical field. The critical electric field required for gap closing decreases with increasing ribbon width, thus the results have practical importance. Further stability analysis shows that bare BeO NRs are more stable than H-passivated BeO NRs of similar ribbon widths and bare armchair BeO NRs are energetically the most favorable among all the nanoribbons.     

Mechanical and magnetic properties of Ni-Co dispersed Al2O3 nanocomposites

Effects of the fabrication processing on the microstructure and properties of composites were investigated. High-density Ni-Co dispersed-Al₂O₃ (Al₂O₃/Ni-Co) composites were obtained by hydrogen reduction and consolidated using hot pressing and pulse electric current sintering (PECS) of Al₂O₃, Ni(NO₃)₂·6H₂O and Co(NO₃)₂·6H₂O powder mixtures. Microstructural investigations of the hot-pressed composite fabricated using again wet/dry ball-milled powder mixture after calcination revealed that fine Ni-Co particles, about 145 nm in diameter, dispersed homogeneously at the matrix grain boundaries. In particular, fine microstructure of dispersion with the average size of 90 nm was realized for the specimen consolidated by PECS method. High strength of over 1 GPa and hardness of 19 GPa were measured for the nanocomposites prepared from the again ball-milled powder mixture. The ferromagnetism of nano-sized Ni-Co contributes to the magnetic properties of the composites. A change in the coercive force with dispersion size was observed. Also, the extent of magnetic response by an applied stress was strongly influenced by the size of Ni-Co particles. The relations between microstructure and mechanical as well as magnetic properties are discussed.     

纳米Ni-20Fe 颗粒增韧Al2O3复合材料的力学性能与磁性能

用机械化学及热压烧结方法成功制备了高致密Ni-20Fe/ Al₂O₃ 纳米复合材料。通过X2ray、FE-SEM、力学性能、磁性能测试, 结果表明, 复合后材料断裂韧性从纯α2Al₂O₃ 相的4. 7 MPa·m1/2 提高到6. 2 MPa·m1/2(19 % (Ni-20Fe) / Al₂O₃ ) , 断裂方式有沿晶断裂和穿晶断裂两种。当Ni-20Fe 合金的体积百分数达到19 %时, 复合材料的饱和磁化强度达33 emu/ g , 矫顽力为200 Oe , 且在低于500 ℃的情况下, 矫顽力基本不随温度而变, 具有良好的磁热稳定性。      

Structure, properties, and thermal stability of nanocrystallite Fe-Ti-N soft magnetic films

We deposited Fe-Ti-N magnetic films with a high sputtering power of 7 W/cm/sup 2/. When the composition of the films was in the range of Fe-Ti(3.9 at.%)-N(8.8 at.%) to Fe-Ti(3.3 at.%)-N(13.5 at.%), the films were composed of /spl alpha/' and Ti/sub 2/N precipitates. With the addition of nitrogen, 4/spl pi/M/sub s/ became higher than that of pure iron, reaching a maximum of 23.8 kG. At the same time, H/sub c/ was reduced to a minimum of 1.12 Oe. The best films can meet the needs of the recording head in dual-element giant magnetoresistive/inductive heads, yielding high storage density (10 Gb/in/sup 2/). The incorporation of N in /spl alpha/-Fe brought about the /spl alpha/' phase with its higher saturation magnetization. Ti additions inhibited the equilibrium decomposition /spl alpha/'/spl rarr//spl alpha/+/spl gamma/'. Because H/sub C//sup D//spl prop/D/sup 6/, where D is average grain diameter, grain size control is very important. The nitrogen induces severe distortion of the /spl alpha/' lattice, which can cause the grains to break into pieces and reduce the grain size. High sputtering power also led to the formation of fine grains, with diameter in the order of 14 nm. Probably Ti/sub 2/N is preferentially precipitated on the grain boundary, pinning the grain boundary and stabilizing the grain size during high-temperature heat treatment. The temperature limit for stability of the structure and its associated low coercivity was not less than 520/spl deg/C.     

Mechanical properties and thermal stability of a Cu-based bulk metallic glass microalloyed with silicon

(Cu₄₂Zr₄₂Al₈Ag₈)_{100? x} Si _x (x?=?0?～?1) amorphous alloy rods of 2–6?mm diameter were prepared by Cu-mold drop casting. The thermal properties, microstructure evolution, and mechanical properties were studied by differential scanning calorimetry (DSC), X-ray diffractometry (XRD), transmission electron microscopy (TEM), hardness test, and compression test. The XRD result revealed that all as-quenched (Cu₄₂Zr₄₂Al₈Ag₈)_100?x Si _x alloy rods exhibited a broad diffraction pattern in the amorphous phase. The (Cu₄₂Zr₄₂Al₈Ag₈)_99.5Si_0.5 alloy was found to possess the highest glass forming ability (GFA) as well as the best thermal stability among all tested samples. In addition, both its hardness and yield strength were increased by the microalloyed Si content. The fracture strength and the plastic strain of (Cu₄₂Zr₄₂Al₈Ag₈)_99.5Si_0.5 amorphous alloy can reach 2000?MPa and 3.5 %.     

Mechanical and thermal properties of physical vapour deposited alumina films Part I Thermal stability

Thermal stability of non-reactive physical vapour deposited alumina films of varying thickness on Al₂O₃-TiC and Si substrates, deposited at two different substrate biases, is examined. Substrate curvature measurements were used to determine the deposition stress and stress development during thermal cycling and annealing. Thermal cycling experiments revealed that the films deposited on Al₂O₃-TiC substrates become irreversibly more compressive on heating and annealing while films deposited on Si substrates become irreversibly more tensile. The deposition stress was found to be independent of film thickness, substrate material, and substrate bias during deposition. The thermal stability was independent of film thickness and substrate bias during deposition.     

Austenitic stainless steels at cryogenic temperatures 1—Structural stability and magnetic properties

The structure and magnetic properties of some 15 austenitic stainless steels were examined after cyclic cooling treatments and low temperature deformation. Magnetic measurements at room temperature, 77 K, and 4.2 K and subsequent metallographic examination suggest that many of the AISI 300 stainless steels such as 301, 302, 303, 304, 304L, 305, 316L, 321, and 347 must be considered potentially unstable with respect to the formation of the ferromagnetic α′ martensite phase on repeated cooling to low temperatures. This structural instability was increased significantly after a sensitizing treatment in the weldable steels 304L, 321, and 347 leading to the formation of up to 11.2% a′ martensite, part of which formed isothermally. Low temperature deformation is even more potent in promoting the transformation, at least 50% α′ martensite being induced by deformation at 4.2 K in the otherwise stable alloys such as 309 and the 0.2% N versions of 304L and 316L. The high alloy steels 310 and Kromarc 55 remain fully a austenitic even after deformation to rupture at 4.2 K. The temperature dependence of the magnetic susceptibility of the latter alloys and Incoloy 800 indicates that their low temperature structural stability is associated with magnetic transitions which occur within the austenite phase.     

Mechanical and magnetic properties of metal fibre networks, with and without a polymeric matrix

Bonded networks of metal fibres are highly porous, permeable materials, which often exhibit relatively high strength. Material of this type has been produced, using melt-extracted ferritic stainless steel fibres, and characterised in terms of fibre volume fraction, fibre segment (joint-to-joint) length and fibre orientation distribution. Young’s moduli and yield stresses have been measured. The behaviour when subjected to a magnetic field has also been investigated. This causes macroscopic straining, as the individual fibres become magnetised and tend to align with the applied field. The modeling approach of Markaki and Clyne, recently developed for prediction of the mechanical and magneto-mechanical properties of such materials, is briefly summarised and comparisons are made with experimental data. The effects of filling the inter-fibre void with compliant (polymeric) matrices have also been explored. In general the modeling approach gives reliable predictions, particularly when the network architecture has been characterised using X-ray tomography.     

磁场诱导定向碳纤维增强水泥砂浆的力学性能

首次利用磁场诱导定向技术,制备了具有明显择优取向的碳纤维增强水泥砂浆,表征与测试了不同水灰比、龄期和纤维掺量的水泥砂浆的碳纤维取向、抗压和劈裂抗拉强度,研究了碳纤维的取向性对力学性能提升效果的影响。结果表明:水灰比、纤维掺量对碳纤维的取向性有显著影响;相较于无择优取向的普通碳纤维增强水泥砂浆,经磁场诱导定向的碳纤维增强水泥砂浆的劈裂抗拉强度有显著增加,而抗压强度无明显变化;相同水灰比下,纤维取向和纤维掺量是影响定向碳纤维增强水泥砂浆劈裂抗拉强度的主要因素。其中,定向碳纤维增强水泥砂浆劈裂抗拉强度增强效率的最佳碳纤维掺量为水泥的0.50%。