88 research outputs found
Effect of laser processing parameters on the structure of ductile iron
Laser processing of structure sensitive hypereutectic ductile iron, a cast alloy employed for dynamically loaded automative components, was experimentally investigated over a wide range of process parameters: from power (0.5-2.5 kW) and scan rate (7.5-25 mm s(-1)) leading to solid state transformation, all the way through to melting followed by rapid quenching. Superfine dendritic (at 10(5) degrees C s(-1)) or feathery (at 10(4) degrees C s(-1)) ledeburite of 0.2-0.25 mu m lamellar space, gamma-austenite and carbide in the laser melted and martensite in the transformed zone or heat-affected zone were observed, depending on the process parameters. Depth of geometric profiles of laser transformed or melt zone structures, parameters such as dendrile arm spacing, volume fraction of carbide and surface hardness bear a direct relationship with the energy intensity P/UDb2, (10-100 J mm(-3)). There is a minimum energy intensity threshold for solid state transformation hardening (0.2 J mm(-3)) and similarly for the initiation of superficial melting (9 J mm(-3)) and full melting (15 J mm(-3)) in the case of ductile iron. Simulation, modeling and thermal analysis of laser processing as a three-dimensional quasi-steady moving heat source problem by a finite difference method, considering temperature dependent energy absorptivity of the material to laser radiation, thermal and physical properties (kappa, rho, c(p)) and freezing under non-equilibrium conditions employing Scheil's equation to compute the proportion of the solid enabled determination of the thermal history of the laser treated zone. This includes assessment of the peak temperature attained at the surface, temperature gradients, the freezing time and rates as well as the geometric profile of the melted, transformed or heat-affected zone. Computed geometric profiles or depth are in close agreement with the experimental data, validating the numerical scheme
Effects of graphene oxide addition on wear behaviour of composite coatings fabricated by plasma electrolytic oxidation (PEO) on AZ91 magnesium alloy
The omega phase formation during laser cladding and remelting of quasicrystal forming AlCuFe on pure aluminum
We report the formation omega phase in the remelted layers during laser cladding and remelting of quasicrystal forming Al65Cu23.3Fe11.7 alloy on pure aluminum. The omega phase is absent in the clad layers. In the remelted layer, the phase nucleates at the periphery of the primary icosahedral phase particles. A large number of omega phase particles forms enveloping the icosahedral phase growing into aluminum rich melt, which solidify as alpha-Al solid solution. On the other side it develops an interface with aluminum. A detailed transmission electron microscopic analysis shows that omega phase exhibits orientation relationship with icosahedral phase. The composition analysis performed using energy dispersive x-ray analyzer suggests that this phase has composition higher aluminum than the icosahedral phase. The analysis of the available phase diagram information indicates that the present results represent large departure from equilibrium conditions. A possible scenario of the evolution of the omega phase has been suggested
Influence of process parameters on the nitriding of steels by plasma immersion ion implantation
Nitriding of steels by Plasma Immersion Ion Implantation (PI3) allows access to a large process parameter space. Although the parameters associated with the high-energy ion bombardment (implantation energy, high-voltage pulse length and frequency, ion current density and time-averaged dose rate) are important, the treatment temperature and plasma parameters such as ion density, excited neutral density and plasma potential also play a vital role. Previous investigations have been hampered by the use of the high-energy ion bombardment to heat the workpiece. In this paper, we present the results of a study in which the treatment temperature and the ion bombardment were decoupled by radiatively heating. The effect of varying high-voltage pulse length, repetition rate, total implanted dose, plasma density and potential on the nitrogen uptake during PI3 treatment depends strongly on whether nitrides are formed in the surface (e.g. Ck45 mild steel) or nitrogen is incorporated in solid solution (e.g. X6CrNiTi 1810 austenitic stainless steel). In the first case, nitride formation can be suppressed by increasing the high-voltage pulse frequency or can be enhanced by treating at a high pressure or plasma potential. In the second case, the thickness of the modified layer can be increased by increasing the ion current density or time-averaged dose rate. In both cases, nitrogen uptake by direct thermochemical absorption from the plasma is significant
Effects of rare earth additions on nitriding of EN40B by plasma immersion ion implantation
Plasma immersion ion implantation of 100Cr6 ball bearing steel
Most low alloy steels are tempered at relatively low temperatures, limiting the opportunities for improving their wear resistance and surface hardness by traditional heat treatment processes. In this work, we use plasma immersion ion implantation (PI3) to apply a hybrid ion implantation/thermochemical diffusion treatment to ball bearing steel 100Cr6 (1% C, 1.5% Cr). By a judicious choice of implantation voltage, temperature and time, it is possible to combine the PI3 treatment with the tempering stage of heat treatment, without compromising the hardness of the alloy. Up to 200 °C, the bulk hardness (750 HV tempered) of the material is maintained, and nitrogen implantation increases the surface hardness due to the precipitation of fine Fe2N. At 300 °C, where enhanced nitrogen and carbon diffusion can occur, the bulk hardness decreases, although in many applications this can be compensated by the increase in surface hardness to around 900 HV0.1 due to Fe3N and Fe4N formation. Wear and corrosion tests reveal significant improvements in comparison with untreated steel
Growth Kinetics Of Γ-Al12Mg17 And Β-Al3Mg2 Intermetallic Phases In Mg Vs. Al Diffusion Couples
Increasing use and development of lightweight Mg-alloys have led to the desire for more fundamental research in and understanding of Mg-based systems. As a strengthening component, Al is one of the most important and common alloying elements for Mg-alloys. In this study, solid-to-solid diffusion couple techniques were employed to examine the interdiffusion between pure Mg and Al. Diffusion anneals were carried out at 300°, 350°, and 400°C for 720, 360, and 240 hours, respectively. Optical and scanning electron microscopies (SEM) were employed to observe the formation of the intermetallics γ-Al12Mg17 and β-Al3Mg2, but not ε-phase. Concentration profiles were determined using X-ray energy dispersive spectroscopy (XEDS). The growth constants and activation energies were determined for each intermetallic phase
Nitrogen and carbon expanded austenite produced by PI3
Expanded austenite can be formed either by nitrogen or carbon plasma immersion ion implantation (PI3 TM) from a nitrogen or methane plasma at elevated temperatures. The structure and properties of nitrogen and carbon expanded austenite layers produced on austenitic stainless steel X5CrNi189 are compared. A new structural model of expanded austenite based on a defect rich face centred cubic (fcc) lattice is proposed. Although the structure of the two expanded austenite layers is similar, there is a remarkable difference in the uptake of nitrogen or carbon, despite the use of similar treatment conditions. The modified surfaces have different hardness, corrosion and wear properties
Surface treatment of nitriding steel 34CrAlNi7: a comparison between pulsed plasma nitriding and plasma immersion ion implantation
A study of the response of the nitriding steel, 34CrAlNi7, to two different nitriding techniques revealed remarkable differences. The techniques used were pulsed plasma nitriding and plasma immersion ion implantation over a range of temperatures from 300 to 500 degrees celsius. The surface produced by the pulsed plasma nitriding consisted of a nitride layer whose thickness varied with temperature, with an underlying diffusion zone. Plasma immersion ion implantation treatment, however, formed nitrides only at the lowest temperature, with most of the nitrogen in solid solution. Although quite different surface structures resulted from the two treatments, similar improvements in wear performance were obtained
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