Nanostructure of pearlitic steels
What is Pearlite ?
The term ‘Pearlite’ or more specific ‘pearlitic steel’ and refers to an iron-based compound phase. The pearlitic microstructure is characterized by the joint arrangement of thin layers of ferrite and cementite.
The often lamellar appearance of pearlite is a bit misleading since the individual lamellae within a pearlite colony are actually inter-connected in three dimensions; a single colony is therefore an interpenetrating bicrystal of ferrite and cementite.
How is pearlite formed ?
Pearlite is formed during sufficiently slow cooling in an iron-carbon system at the eutectoid point in the Fe-C phase diagram (723 °C, eutectoid temperature). In a pure Fe-C alloy it contains about 88 vol.% ferrite and 12 vol.% cementite. Pearlite is known for being tough and, when highly deformed, extremely strong.
What is the structure of pearlite ?
Currently pearlitic steels are the strongest and yet ductile commercial bulk materials one earth. When studied under a microscope, it has a very distinctive appearance created by the thin lamellar bands. The term ‘pearlite’ is a reference to the appearance of this alloy phase when studied under the microscope. It resembles mother of pearl (nacre), a natural lamellar structure seen among some shellfish. However, one should not that mother of pearl is created through the natural deposition of successive layers, rather than as the result of special treatment of a eutectoid mixture, but it shares the trait of hardness and strength created by thin subsequent layers of material.
Who discovered pearlite?
Pearlite was first identified by Henry Clifton Sorby and hence it was initially named sorbite, however the similarity of microstructure to nacre and especially the optical effect caused by the scale of the structure made the alternative name 'pearlite' more popular.
How can segregation assist in stabilizing nanocrystalline materials - here specifically in pearlite ?
Grain refinement through severe plastic deformation enables synthesis of ultrahigh-strength nanostructured materials. Two challenges exist in that context: First, deformation-driven grain
refinement is limited by dynamic dislocation recovery and crystal coarsening due to capillary driving forces; second, grain boundary sliding and hence softening occur when the grain size
approaches several nanometers. Here, both challenges have been overcome by severe drawing of a pearlitic steel wire (pearlite: lamellar structure
of alternating iron and iron carbide layers). First, at large strains the carbide phase dissolves via mechanical alloying, rendering the initially two-phase pearlite structure into a carbon-supersaturated iron phase. This carbon-rich iron phase evolves into a columnar nanoscaled subgrain structure which topologically prevents grain boundary sliding. Second, Gibbs segregation of the supersaturated carbon to the iron subgrain boundaries reduces their interface energy, hence reducing the driving force for dynamic recovery and
crystal coarsening. Thus, a stable cross-sectional subgrain size < 10 nm is achieved. These two effects lead to a stable columnar nanosized grain structure that impedes dislocation motion and enables an extreme
tensile strength of 7 GPa, making this alloy the strongest ductile bulk material known.
PRL 113, 106104 (2014)
Phys Rev Lett vol 113 page 106104 (2014)[...]
PDF-Dokument [2.2 MB]
How can we make ultra-strong and damage tolerant metallic bulk materials?
Structural materials used for safety critical applications require high strength and simultaneously high resistance against crack growth, referred to as damage tolerance. However, the two
properties typically exclude each other and research efforts towards ever stronger materials are hampered by drastic loss of fracture resistance. Therefore, future development of novel
ultra-strong bulk materials requires a fundamental understanding of the toughness determining mechanisms. As model material we use today’s strongest metallic bulk material, namely, a
nanostructured pearlitic steel wire, and measured the fracture toughness on micron-sized specimens in different crack growth directions and found an unexpected strong anisotropy in the
fracture resistance. Along the wire axis the material reveals ultrahigh strength combined with so far unprecedented damage tolerance. We attribute this excellent property combination to the
anisotropy in the fracture toughness inducing a high propensity for microcrack
formation parallel to the wire axis. This effect causes a local crack tip stress relaxation and enables the high fracture toughness without being detrimental to the material’s strength.
Scientific Reports 6, Article number: 33228 (2016)
Ultrastrong damage tolerant Scientific R[...]
PDF-Dokument [1.7 MB]
How can we measure grain boundary segregation in nanocrystalline material at the atomic-scale ?
Grain boundary segregation leads to nanoscale chemical variations that can alter a material's performance by orders ofmagnitude (e.g., embrittlement). To understand this phenomenon, a large
number of grain boundaries must be characterized in terms of both their five crystallographic interface parameters and their atomic-scale chemical composition. We demonstrate how this can
be achieved using an approach that combines the accuracy of structural characterization in transmission electron microscopy with the 3D chemical sensitivity of atom probe tomography.We find
a linear trend between carbon segregation and the misorientation angle ω for low-angle grain boundaries in ferrite, which indicates that ω is the most influential crystallographic
in this regime. However, there are significant deviations from this linear trend indicating an additional strong influence of other crystallographic parameters (grain boundary plane, rotation axis). For high-angle grain boundaries, no general trend between carbon excess and ω is observed; i.e., the grain boundary plane and rotation axis have an even higher influence on the segregation behavior in this regime. Slight deviations from special grain boundary configurations are shown to lead to unexpectedly high levels of segregation.
PRL 112, 126103 (2014)
PDF-Dokument [842.8 KB]
In order to investigate the thermodynamic driving force for the experimentally observed accumulation of C in ferritic layers of severely plastically deformed pearlitic wires, the stabilities of C inte
Acta Mater 61 (2013) 1773-solute-C-in-pe[...]
PDF-Dokument [1.0 MB]
Acta Materialia 84 (2015) 110-123
Acta Materialia 84 (2015) 110-123 atom p[...]
PDF-Dokument [2.4 MB]
Carbon-supersaturated nanocrystalline hypereutectoid steels with a tensile strength of 6.35 GPa were produced from severely cold-drawn pearlite. The nanocrystalline material undergoes softening upon annealing at temperatures between 200 and 450°C. The ductility in terms of elongation to failure exhibits a non-monotonic dependence on temperature. Here, the microstructural mechanisms responsible for changes in the mechanical properties were studied using transmission electron microscopy (TEM), TEM-based automated scanning nanobeam diffraction and atom probe tomography (APT). TEM and APT investigations of the nanocrystalline hypereutectoid steel show subgrain coarsening upon annealing, which leads to strength reduction following a Hall–Petch law. APT analyzes of the Mn distribution near subgrain boundaries and in the cementite give strong evidence of capillary-driven subgrain coarsening occurring through subgrain boundary migration. The pronounced deterioration of ductility after annealing at temperatures above 350 °C is attributed to the formation of cementite at subgrain boundaries. The overall segregation of carbon atoms at ferrite subgrain boundaries gives the nanocrystalline material excellent thermal stability upon annealing.
Acta Materialia 59 (2011) 3965-3977
Y.J. Li, P. Choi, C. Borchers, S. Westerkamp, S. Goto, D. Raabe, R. Kirchheim
Atomic-scale mechanisms of deformation-induced cementite decomposition in pearlite
Acta Materialia 59 (2011) 3965 pearlite [...]
PDF-Dokument [1.0 MB]
Pearlitic steel can exhibit tensile strengths higher than 5 GPa after severe plastic deformation, where the deformation promotes a refinement of the lamellar structure and cementite
decomposition. However, a convincing correlation between deformation and cementite decomposition in pearlite is still absent. In the present work, a local electrode atom probe was used to
characterize the microstructural evolution of pearlitic steel, cold-drawn with progressive strains up to 5.4. Transmission electron microscopy was also employed to perform complementary
analyses of the microstructure. Both methods yielded consistent results. The overall carbon content in the detected
volumes as well as the carbon concentrations in ferrite and cementite were measured by atom probe. In addition, the thickness of the cementite filaments was determined. In ferrite, we found a correlation of carbon concentration with the strain, and in cementite, we found a correlation of carbon concentration with the lamella thickness. Direct evidence for the formation of cell/subgrain boundaries in ferrite and segregation of carbon atoms at these defects was found. Based on these findings, the mechanisms of cementite decomposition
are discussed in terms of carbon–dislocation interaction.
Acta Materialia 60 (2012) 4005-4016
Acta mater Vol 60 2012-heat treated pear[...]
PDF-Dokument [2.7 MB]
Hypereutectoid steel wires with 6.35 GPa tensile strength after a cold-drawing true strain of 6.02 were annealed between 300 and 723 K. The ultrahigh strength remained upon annealing for 30 min up to a temperature of 423 K but dramatically decreased with further increasing temperature. The reduction of tensile strength mainly occurred within the first 2–3 min of annealing. Atom probe tomography and transmission electron microscopy reveal that the lamellar structure remains up to 523 K. After annealing at 673 K for 30 min, coarse hexagonal ferrite (sub)grains with spheroidized cementite, preferentially located at triple junctions, were observed in transverse cross-sections. C and Si segregated at the (sub)grain boundaries, while Mn and Cr enriched at the ferrite/cementite phase boundaries due to their low mobility in cementite. No evidence of recrystallization was found even after annealing at 723 K for 30 min. The stability of the tensile strength for low-temperature annealing (<473 K) and its dramatic drop upon high-temperature annealing (>473 K) are discussed based on the nanostructural observations.
small overview paper by: D. Raabe, P. P. Choi, Y.J. Li, A. Kostka, X. Sauvage, F. Lecouturier, K. Hono, R. Kirchheim, R. Pippan, D. Embury: MRS Bulletin 35 (2010) 982-991
PDF-Dokument [2.2 MB]
Atom probe analysis of interfaces in pearlite: Lecture by Y. Li, S. Goto, C. Borchers*, P. Choi, M. Herbig, S. Zaefferer, A. Kostka, J. von Pezold, A. Nematollahi, J. Neugebauer, R. Kirchheim, D. Raab
PDF-Dokument [1.6 MB]
Pearlite microstructures observed by EBSD in 2D EBSD and 3D EBSD
The microstructure of pearlite in hypoeutectoid steel was investigated using high resolution orientation imaging microscopy. Systematic orientation gradients were observed along the longitudinal direc
steel research int. 78 (2007) perlite te[...]
PDF-Dokument [310.6 KB]
Metallurgical and Mater Trans A vol 39A [...]
PDF-Dokument [1.0 MB]