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Showing papers on "Bainite published in 2011"


Journal ArticleDOI
TL;DR: In this paper, three ferrite/martensite dual-phase steels varying in the ferrite grain size (12.4, 2.4 and 1.2μm) but with the same martensite content (∼30 vol%) were produced by large-strain warm deformation at different deformation temperatures, followed by intercritical annealing.

590 citations


Journal ArticleDOI
TL;DR: In this paper, the authors report on the microstructure, texture and deformation mechanisms of a novel ductile lean duplex stainless steel (Fe 19.9Cr 0.42Ni 0.16N 4.35Si, wt.

405 citations


Journal ArticleDOI
TL;DR: In this paper, a family of transformation-induced plasticity (TRIP) steels with varying retained austenite contents was used to produce a series of transformation induced plasticity steels for cold-rolled 0.1C-7.1Mn steel.
Abstract: Manganese enrichment of austenite during prolonged intercritical annealing was used to produce a family of transformation-induced plasticity (TRIP) steels with varying retained austenite contents. Cold-rolled 0.1C-7.1Mn steel was annealed at incremental temperatures between 848 K and 948 K (575 °C and 675 °C) for 1 week to enrich austenite in manganese. The resulting microstructures are comprised of varying fractions of intercritical ferrite, martensite, and retained austenite. Tensile behavior is dependent on annealing temperature and ranged from a low strain-hardening “flat” curve to high strength and ductility conditions that display positive strain hardening over a range of strain levels. The mechanical stability of austenite was measured using in-situ neutron diffraction and was shown to depend significantly on annealing temperature. Variations in austenite stability between annealing conditions help explain the observed strain hardening behaviors.

310 citations


Journal ArticleDOI
TL;DR: In this article, a detailed characterization of the microstructural development of a new quenching and partitioning (Q&P) steel was presented, which showed that stabilization of austenite can be achieved at significantly shorter time scales via the Q&P route than is possible via a bainitic isothermal holding.

266 citations


Journal ArticleDOI
TL;DR: In this article, a local electrode atom probe was used to characterize the microstructural evolution of pearlitic steel, cold-drawn with progressive strains up to 5.4 GPa.

257 citations


Journal ArticleDOI
TL;DR: In this paper, the authors present atom probe tomography results across martensite/austenite interfaces in a precipitation-hardened MARaging-TRIP steel (12.2 Mn, 1.9 Ni, 0.6 Mo, 1 2 Ti, 0 3 Al; at%).

251 citations


Journal ArticleDOI
TL;DR: In this article, two distinct TRIP steel microstructures, equiaxed versus lamellar, and how microstructure affects the retained austenite transformation during uniaxial tensile loading were investigated.
Abstract: Retained austenite is a metastable phase in transformation induced plasticity (TRIP) steels that transforms into martensite under local stress and strain. This transformation improves sheet formability, allowing this class of higher strength steels to be used for applications such as automotive structural components. The current work studies two distinct TRIP steel microstructures, i.e. equiaxed versus lamellar, and how microstructure affects the austenite transformation during uniaxial tensile loading. Different heat treatments were employed to obtain the two microstructures, and the bainite hold times of the treatments were varied to change the volume fraction of retained austenite. Based on uniaxial tensile response and magnetic saturation measurements, the bainite hold time of 100 s was determined to produce the best results in terms of largest strain at the ultimate tensile strength and highest volume fraction of retained austenite. The work hardening of the samples with a 100 s bainite hold was evaluated by calculating the instantaneous n value as a function of strain. It was found that the lamellar microstructure has a lower maximum instantaneous n value than the equiaxed microstructure, but has higher work hardening values for strain levels greater than 0.05 and up to the ultimate tensile strength. This difference in work hardening behaviour corresponds directly to the transformation rate of retained austenite in the two microstructures. The slower rate of transformation in the lamellar microstructure allows for work hardening to persist at high strains where the transformation effect has already been exhausted in the equiaxed microstructure. The different rates of transformation can be attributed to the location, carbon content, and size of the retained austenite grains in the respective TRIP microstructures.

239 citations


Journal ArticleDOI
TL;DR: In this article, the authors investigated the correlation of microstructural characteristics and toughness of the simulated coarse grained heat affected zone (CGHAZ) of low carbon bainitic steel.
Abstract: The correlation of microstructural characteristics and toughness of the simulated coarse grained heat affected zone (CGHAZ) of low carbon bainitic steel was investigated in this study. The toughness of simulated specimens was examined by using an instrumented Charpy impact tester after the simulation welding test was conducted with different cooling times. Microstructure observation and crystallographic feature analysis were conducted by means of optical microscope and scanning electron microscope equipped with electron back scattered diffraction (EBSD) system, respectively. The main microstructure of simulated specimen changes from lath martensite to coarse bainite with the increase in cooling time. The deterioration of its toughness occurs when the cooling time ranges from 10 to 50 s compared with base metal toughness, and the toughness becomes even worse when the cooling time increases to 90 s or more. The MA (martensite–austenite) constituent is primary responsible for the low toughness of simulated CGHAZ with high values of cooling time because the large MA constituent reduces the crack initiation energy significantly. For crack propagation energy, the small effective grain size of lath martensite plays an important role in improving the crack propagation energy. By contrast, high misorientation packet boundary in coarse bainite seems to have few contributions to the improvement of the toughness because cleavage fracture micromechanism of coarse bainite is mainly controlled by crack initiation.

217 citations


Journal ArticleDOI
TL;DR: In this paper, a model was proposed to predict Austenite stabilization through manganese partitioning between ferrite and austenite, and the model predicts retainedAustenite fractions as a function of intercritical annealing temperature based on equilibrium phase fractions and solute contents.

216 citations


Journal ArticleDOI
TL;DR: In this article, deformation dilatometry has been used to simulate controlled hot rolling followed by cooling of a Nb-V low carbon steel, looking for conditions corresponding to wide austenite grain size distributions prior to transformation.
Abstract: Deformation dilatometry has been used to simulate controlled hot rolling followed by cooling of a Nb–V low carbon steel, looking for conditions corresponding to wide austenite grain size distributions prior to transformation. Recrystallization and non-recrystallization deformation schedules were applied, followed by controlled cooling at rates from 0.1 °C/s to about 200 °C/s, and the corresponding continuous cooling transformation (CCT) diagrams were constructed. The resultant microstructures ranged from polygonal ferrite (PF) and pearlite (P) at slow cooling rates to bainitic ferrite (BF) accompanied by martensite (M) for fast cooling rates. Plastic deformation of the parent austenite accelerated both ferrite and bainite transformations, displacing the CCT curve to higher temperatures and shorter times. However, it was found that the accelerating effect of strain on bainite transformation weakened as the cooling rate diminished and the polygonal ferrite formation was enhanced. Moreover, it was found that plastic deformation had different effects on the refinement of the microstructure, depending on the cooling rate. An analysis of the microstructural heterogeneities that can impair toughness behavior has been done.

143 citations


Journal ArticleDOI
TL;DR: In this paper, a cold-rolled dual-phase (DP) steel based on a low-carbon DP780 composition processed in the mill was investigated using two heating rates, 10 and 50 K/s, and a range of annealing temperatures from 1053 K to 1133 K (780 −C to 860 −C) to study their effects on the progress of austenitization.
Abstract: Austenite formation during intercritical annealing was studied in a cold-rolled dual-phase (DP) steel based on a low-carbon DP780 composition processed in the mill. Two heating rates, 10 and 50 K/s, and a range of annealing temperatures from 1053 K to 1133 K (780 °C to 860 °C) were applied to study their effects on the progress of austenitization. The effect of these process parameters on the final microstructures and mechanical properties was also investigated using a fixed cooling rate of 10 K/s after corresponding annealing treatments. It was found that the heating rate affects the austenite formation not only during continuous heating, but also during isothermal holding, and the effect is more pronounced at lower annealing temperatures. Faster heating delays the recrystallization kinetics of the investigated steel. The rate of austenite formation and its distribution are strongly influenced by the extent of overlapping of the processes of recrystallization and austenitization. It appeared that the heating rate and temperature of intercritical annealing have a stronger effect on the final tensile strength (TS) of the DP steel than holding time. Both higher annealing temperatures and long holding times minimize the strength difference caused by a difference in heating rate.

Journal ArticleDOI
P. Zhang1, F.C. Zhang1, Zhigang Yan1, T.S. Wang1, Lihe Qian1 
22 Jun 2011-Wear
TL;DR: In this paper, a process primarily based on carburization and successive low-temperature austempering, was proposed for the generation of low temperature bainitic microstructure in the surface layer (∼2.5mm in thickness) of low carbon steel.

Journal ArticleDOI
TL;DR: In this article, the authors provide an overview on the application of phase field models to describe microstructure evolution in steels, focusing on phase field modeling of the austenite-ferrite transformation.
Abstract: This article provides an overview on the application of phase field models to describe microstructure evolution in steels. The focus will be on phase field modeling of the austenite–ferrite transformation as this has emerged as a particularly active area of research in the past few years. Phase field models are powerful tools to deal with the complex morphologies, e.g. Widmanstatten ferrite, that may result from these transformations. Even though much progress has been attained there is still significant work to be done in applying these models to processing of advanced steels with complex multi-phase microstructures. In particular, the phase field approach promises to have significant impact on modeling of bainite formation and the microstructure evolution in the heat affected zone of welds.

Journal ArticleDOI
TL;DR: In this article, phase-formation based concepts for the design of quenching and partitioning (Q&P) steels are evaluated. But the authors focus on the first quench step and the formation of bainite, carbides, and carbon gradients as well as migration of martensite/austenite interfaces.
Abstract: The application of the quenching and partitioning (Q&P) process in steels involves a microstructural evolution that is more complex than just the formation of martensite followed by carbon partitioning from martensite to austenite. Examples of this complexity are the formation of epitaxial ferrite during the first quenching step and the formation of bainite, carbides, and carbon gradients as well as migration of martensite/austenite interfaces during the partitioning step. In this work, recent investigations on the mechanisms controlling microstructural changes during the application of the Q&P process are evaluated, leading to phase-formation based concepts for the design of Q&P steels.

Journal ArticleDOI
TL;DR: In this article, the microstructural evolution of Fe 0.2C-5Mn steel during intercritical annealing with holding time for up to 144 hours was examined by TEM and STEM.
Abstract: The microstructural evolution of Fe–0.2C–5Mn steel during intercritical annealing with holding time for up to 144 hours was examined by TEM and STEM. It was demonstrated by TEM that the martensite lath structure gradually transformed into a lamellar ferrite and austenite duplex structure. The partitioning of manganese from ferrite to austenite was found by STEM. Typical Kurdjumov-Sachs orientation relationship between austenite lath and ferrite lath was observed by electron back scattered diffraction (EBSD). Based on the analysis of the austenite lath thckening behavior, it was proposed that the Mn-partitioning in austenite dominated the microstructure evolution of the ultrafine lamellar ferrite and austenite duplex structure during annealing process.

Journal ArticleDOI
TL;DR: In this paper, a 0.79 C-1.58 Co (wt.%) steel was isothermally heat treated at 200 and 350°C for one day to form a nanoscale bainitic microstructure consisting of nanobainitic ferrite laths with high dislocation density.

Journal ArticleDOI
TL;DR: In this paper, a steel microstructure with a high tensile strength and good ductility similar to that of advanced high strength steels was constructed using flash processing of an AISI8620 steel sheet, which involves rapid heating and cooling with an overall process duration of <10 s.
Abstract: Flash processing of an AISI8620 steel sheet, which involves rapid heating and cooling with an overall process duration of <10 s, produced a steel microstructure with a high tensile strength and good ductility similar to that of advanced high strength steels. Flash processed steel [ultimate tensile strength (UTS): 1694 MPa, elongation: 7·1%], showed at least 7% higher UTS and 30% greater elongation than published results on martensitic advanced high strength steel (UTS: 1585 MPa, elongation: 5·1%). The underlying microstructure was characterised with optical, scanning electron, transmission electron microscopy as well as hardness mapping. A complex distribution of bainitic and martensite microstructures with carbides was observed. A mechanism for the above microstructure evolution is proposed.

Journal ArticleDOI
TL;DR: In this paper, the influence of tempering temperature on the reversed austenite formation and tensile properties is investigated in Fe-13%Cr-4%Ni-Mo low carbon martensite stainless steel in the temperature range of 550-950 degrees C.
Abstract: The influence of tempering temperature on the reversed austenite formation and tensile properties are investigated in Fe-13%Cr-4%Ni-Mo low carbon martensite stainless steel in the temperature range of 550-950 degrees C. It is found that at the temperatures below 680 degrees C, the reversed austenite formation occurs by diffusion. Amount of the reversed austenite is determined I:IN the tempering temperature and the holding time. The segregation of Ni is the main reason for the stability of the reversed austenite. When the temperatures are above 680 degrees C, the reversed austenite formation proceeds by diffusionless. The reversed austenite will transform back to martensite after cooled to room temperature. The tensile properties are most strongly influenced by the amount of the reversed austenite obtained at room temperature. The excellent combination of good strength and ductility is at 610 degrees C. (C) 2011 Elsevier B.V. All rights reserved.

Journal ArticleDOI
TL;DR: In this article, the authors studied structure-property correlations in a weld overlay clad high strength low alloy steel with austenitic stainless steel of American Institute for Steel and Iron (AISI) 347 grade.

Journal ArticleDOI
TL;DR: The microstructures and mechanical properties of Cr13 super martensitic stainless steel after different heat treatments were studied in this paper, which showed that the structures of the steel after quenching are of lath martensite mixed with a small amount of retained austenite.
Abstract: The microstructures and mechanical properties of Cr13 super martensitic stainless steel after different heat treatments were studied. The results show that the structures of the steel after quenching are of lath martensite mixed with a small amount of retained austenite. With the raising quenching temperature, the original austenite grain size increases and the lath martensite gradually becomes thicker. The structures of the tempered steel are mixtures of tempered martensite and reversed austenite dispersed in the martensite matrix. The amount of reversed austenite is from 7.54% to 22.49%. After different heat treatments, the tensile strength, the elongation and the HRC hardness of the steel are in the range of 813–1070 MPa, 10.1%–21.2% and 21.33–32.37, respectively. The steel displays the best comprehensive mechanical properties after the sample is quenched at 1050 °C followed by tempering at 650 °C.

Journal ArticleDOI
TL;DR: In this paper, the tempering of two-phase mixtures of bainitic ferrite and carbon-enriched retained austenite has been investigated in an effort to separate the reactions that occur at elevated temperatures from any transformation during cooling to ambient conditions.
Abstract: The tempering of two-phase mixtures of bainitic ferrite and carbon-enriched retained austenite has been investigated in an effort to separate the reactions that occur at elevated temperatures from any transformation during cooling to ambient conditions. It is demonstrated using synchrotron X-radiation measurements that the residue of austenite left at the tempering temperature partly decomposes by martensitic transformation when the sample is cooled. It is well established in the published literature that films of retained austenite are better able to resist stress or strain-induced martensitic transformation than any coarser particles of austenite. In contrast, the coarser austenite is more resistant to the precipitation of cementite during tempering than the film form because of its lower carbon concentration.

Journal ArticleDOI
TL;DR: In this paper, the authors demonstrate that a large amount of published data relating the fraction of martensite to plastic strain can in fact be described in terms of the pure thermodynamic effect of applied stress.
Abstract: Many studies monitoring the formation of martensite during the tensile deformation of austenite report data which are, in principle, affected by both the applied stress and the resulting plastic strain. It is not clear in these circumstances whether the transformation is stress induced (i.e. the stress provides a mechanical driving force) or whether the generation of defects during deformation helps nucleate martensite in a scenario better described as strain induced transformation. The authors demonstrate in the present work that a large amount of published data relating the fraction of martensite to plastic strain can in fact be described in terms of the pure thermodynamic effect of applied stress.

Journal ArticleDOI
TL;DR: In this paper, the temperature dependence of austenite nucleation behavior was investigated in an ultralow carbon 13%Cr 6%Ni martensitic stainless steel, and the transition of nucleation site was discussed in terms of energy by considering the increases in interfacial energy and elastic strain energy by formation of an Austenite nucleus.
Abstract: The temperature dependence of austenite nucleation behavior was investigated in an ultralow carbon 13%Cr–6%Ni martensitic stainless steel. The martensitic structure was partially reversed to austenite by heat treatment at different temperature in (austenite+ferrite) two-phase region. With increasing the reversion temperature, the shape of austenite grains tend to be changed from acicular to granular, and their nucleation site is changed from lath boundaries to prior austenite grain boundaries. The transition of nucleation site was discussed in terms of energetics by considering the increases in interfacial energy and elastic strain energy by formation of an austenite nucleus. The calculation results suggested that lath boundary is more preferential nucleation site rather than prior austenite grain boundary because the increment of elastic strain energy is reduced with lowing the reversion temperature.

Journal ArticleDOI
TL;DR: In this paper, high-resolution transmission electron microscopy and atom probe tomography have provided new experimental evidence on the accommodation of transformation strain, a subject critically relevant to understanding the atomic mechanisms controlling bainitic ferrite growth.

Journal ArticleDOI
TL;DR: In this paper, a new processing technique was proposed in which the hot stamping step is followed by a controlled quenching and partitioning process, producing a microstructure containing retained austenite and martensite.

Journal ArticleDOI
TL;DR: In this article, the size distribution and structural properties of (Nb,Ti)N and NbC precipitates, their occurrence in the various steel phases, and their relationship with the Fe matrix were investigated.

Journal ArticleDOI
01 Jun 2011
TL;DR: In this paper, a component prepared by shaped metal deposition (SMD) using 300M steel wire is studied to reveal structure and material properties, which exhibits a bainitic microstructure changing from distinct sheaves to homogenous from top to bottom.
Abstract: A component prepared by shaped metal deposition (SMD) using 300M steel wire is studied to reveal structure and material properties. The component exhibits a bainitic microstructure changing from distinct sheaves to homogenous from top to bottom. This change in microstructure is reflected by a step-like increase of the volume fraction of austenite towards the bottom of the component, and a step-like decrease of the microhardness. A certain deviation of the general change in the morphology of bainite from top to bottom appears at the very bottom of the component, caused by the influence of the base plate. Tensile tests show a very high ultimate tensile strength of about 1500 MPa and an elastic modulus of 200 GPa, which is comparable to that of material in cast condition.

Patent
28 Feb 2011
TL;DR: In this paper, the authors obtained a high-strength pressed member having a tensile strength of at least 980 MPa and excellent ductility of TS×T by means of: the composition of the steel sheet configuring the member containing, by mass, at least 0.12% and no more than 0.69% C.
Abstract: The disclosed method obtains a high-strength pressed member having a tensile strength of at least 980 MPa and excellent ductility of TS×T.EL ≥ 17000 (MPa∙%) by means of: the composition of the steel sheet configuring the member containing, by mass, at least 0.12% and no more than 0.69% C, no more than 3.0% Si, at least 0.5% and no more than 3.0% Mn, no more than 0.1% P, no more than 0.07% S, no more than 3.0% Al, and no more than 0.010% N, Si + Al being at least 0.7% and the remainder being Fe and unavoidable impurities; the structure of the steel sheet configuring the member having martensite, residual austenite, and bainite containing bainitic ferrite; the area ratio of said martensite to the total steel sheet structure being at least 10% and no more than 85%; at least 25% of said martensite being tempered martensite; the amount of said residual austenite being at least 5% and no more than 40%; the area ratio of bainitic ferrite in said bainite to the total steel sheet structure being at least 5%; the total of the area ratio of said martensite, the area ratio of said residual austenite, and the area ratio of said bainitic ferrite in the bainite to the total steel sheet structure being at least 65%; and the average amount of C in the residual austenite being at least 0.65%.

Journal ArticleDOI
TL;DR: In this paper, the temperature dependence of the martensite formation and the mechanical properties of three high alloyed Cr-Mn-Ni as-cast steels with varying Ni contents were studied.
Abstract: The temperature dependence of the martensite formation and the mechanical properties of three high alloyed Cr-Mn-Ni as-cast steels with varying Ni contents were studied. The results showed that the Ms and Md temperatures of the steels decrease with increasing nickel contents. Therefore the strain-induced martensite formation, the TRIP effect and the temperature anomaly of the elongations occurs at lower temperatures. The steel alloyed with 3% nickel shows a stress induced formation of martensite and a dynamic strain aging. Depending on the nickel content and the temperature a TWIP effect occurs additionally to the TRIP effect in the investigated steels. The study was performed by using static tensile tests, dilatometer tests, optical microscopy and the magnetic scale for the detection of ferromagnetic phase fractions.

Journal ArticleDOI
TL;DR: In this article, the effective surface area of cleavage fracture γ p is determined for each microstructural unit, and it is concluded that the bainite packet size determined by EBSD with a 15° misorientation angle criterion is the micro-structural parameter that controls cleavage crack propagation.
Abstract: For a bainitic steel of C = 0.38%, the bainitic packet size measured by OM is about 3.5 times larger than that measured by EBSD with a 15° grain boundary misorientation. This ratio is used to calculate the effective surface energy given by Griffith's model for cleavage fracture. Average ferrite lath width and cementite carbide width values are also measured. Following the general form of Griffith's equation, the effective surface area of cleavage fracture γ p is determined for each microstructural unit. It is concluded that the bainite packet size determined by EBSD with a 15° misorientation angle criterion is the microstructural parameter that controls cleavage crack propagation. Given the relationship between the average unit crack path (UCP) and the bainitic packet size, it is concluded that the effective surface energy of cleavage fracture ( γ p ) is between 71.6 and 82.6 J m −2 .