Abstract:We report on the characterization of high carbon bearing steel 100Cr6 using electron microscopy and atom probe tomography in combination with multi-component diffusion simulations. Scanning electron micrographs show that around 14 vol pct spheroidized carbides are formed during soft annealing and only 3 vol pct remain after dissolution into the austenitic matrix through austenitization at 1123 K (850°C) for 300 seconds. The spheroidized particles are identified as (Fe, Cr) 3 C by transmission electron microsco… Show more
“…The average volume fraction of carbides is 15.9 pct, which is slightly larger compared with the measured value by Song et al [25] That is mainly due to the larger carbon content of the experimental steel in this work. [26] In addition, there may exist statistical error.…”
In order to control the size and distribution of carbides and improve the cold formability of 1.0C-1.5Cr bearing steel, the effects of annealing parameters during isothermal spheroidization were studied. Mean diameter of carbides (D), interparticle spacing of carbides (s), number of carbides per area (n), and carbides particle size distribution were measured. The cold formability was evaluated through hardness and fracture strain. The results show that when austenitizing time increases from 0.5 to 7 hours or austenitizing temperature increases from 1033 K to 1153 K (760°C to 880°C), the values of D and s both increase, and the value of n decreases. With the increasing of second annealing time from 0.5 to 2 hours or the increasing of second annealing temperature from 953 K to 993 K (680°C to 720°C), the values of D and s tend to increase and the value of n decreases. According to the measured values of D, s, and n, two models describing their relationships were proposed. In addition, the hardness decreases with the increasing of D. The fracture strain changes slightly at first and then decreases significantly when the value of D exceeds 0.36 lm.
“…The average volume fraction of carbides is 15.9 pct, which is slightly larger compared with the measured value by Song et al [25] That is mainly due to the larger carbon content of the experimental steel in this work. [26] In addition, there may exist statistical error.…”
In order to control the size and distribution of carbides and improve the cold formability of 1.0C-1.5Cr bearing steel, the effects of annealing parameters during isothermal spheroidization were studied. Mean diameter of carbides (D), interparticle spacing of carbides (s), number of carbides per area (n), and carbides particle size distribution were measured. The cold formability was evaluated through hardness and fracture strain. The results show that when austenitizing time increases from 0.5 to 7 hours or austenitizing temperature increases from 1033 K to 1153 K (760°C to 880°C), the values of D and s both increase, and the value of n decreases. With the increasing of second annealing time from 0.5 to 2 hours or the increasing of second annealing temperature from 953 K to 993 K (680°C to 720°C), the values of D and s tend to increase and the value of n decreases. According to the measured values of D, s, and n, two models describing their relationships were proposed. In addition, the hardness decreases with the increasing of D. The fracture strain changes slightly at first and then decreases significantly when the value of D exceeds 0.36 lm.
“…By using metallographic methods (i.e., grinding, polishing, Klemm etching and analysis of the following image by contrast), the volume fraction of carbides is estimated from the area fraction in the SEM images by the measuring of 2000 particles. This yielded 14 vol% and 3 vol% before and after austenitization, respectively [4]. During austenitization, the average carbide size decreases from 0.63 ± 0.02 µm to 0.49 ± 0.02 µm.…”
Section: Metallography and Microstructurementioning
confidence: 95%
“…Lath martensite consists of fine hierarchically arranged laths with a thickness of 100-300 nm. Laths are characterized by containing a high dislocation density with carbon enrichment at the dislocations via Cottrell atmospheres [4]. The dislocation density as a function of carbon content has been predicted in a previous study and it will be used to estimate the strain energy accommodated by laths [14].…”
Section: Strain Energy Accommodated By Martensite Laths and Plates Inmentioning
confidence: 98%
“…As shown in Figure 2b,d, the spheroidized particles become smaller and more spherical after quenching. The partially dissolved spheroidized carbides have been identified in a previous study [4] to be (Fe, Cr)3C by employing TEM for crystallographic analysis with the zone direction of [011] using the method of SAD (Selected Area Diffraction) and APT for the identification of chemical composition.…”
Section: Metallography and Microstructurementioning
confidence: 99%
“…The atom probe tomography investigations of the lath-structured martensite revealed localized carbon concentrations of 12-14 at%. Clustering was attributed to the segregation of carbon to dislocations and the formation of Cottrell atmospheres despite significant higher carbon concentrations in comparison to the reported values of 6-8 at% [4,5]. Li et al [6] studied the influence of rolling contact loading on the plate-like martensitic microstructure and the resulting distributions of the major alloying elements C and Cr using atom probe tomography.…”
Abstract:The microstructure of the as-quenched plate martensite in a high-C steel 100Cr6 was characterized by means of electron microscopy and atom probe tomography. The carbon redistribution behavior was investigated at the atomic scale, which revealed the nature of the transformation dynamics influenced by carbon and other substitutional alloying elements. A model was proposed to predict the carbon redistribution at twins and dislocations in martensite, which was based on their spatial arrangements.
The industrial process for the production of fine‐blanking steels, which includes hot‐rolling, cold‐rolling, and spheroidizing annealing, is simulated at a laboratory scale using two medium carbon steels, respectively, microalloyed with Cr and Nb. Two types of hot‐rolled microstructures, that is, “ferrite + pearlite” and bainite are obtained by varying the interrupted cooling temperature (ICT). The microstructure and property evolution during spheroidizing annealing are characterized by scanning electron microscopy (SEM), transmission electron microscopy (TEM), electron back scattered diffraction (EBSD), and micro‐hardness tester. In Cr microalloyed steel, the dual partitioning of Cr and Mn and slowed growth kinetics of cementite particle are correlated to explain the suppression of ferrite recrystallization. Contrarily, a fast spheroidizing annealing behavior, which led to uniform distribution of cementite particle and fully recrystallized ferritic matrix, is observed in Nb microalloyed steel especially from the hot‐rolled bainite microstructure.
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