1. Introduction
The wear resistance of tool steels depends upon the microstructure, including the spacing, size, and type of hard particles, as well as the ability of the matrix to absorb energy, all defining steel hardness and toughness [
1].
Carbide-free bainitic microstructures are known to exhibit superior combination of mechanical and wear resistant properties. This is provided by the very fine scale of bainitic ferrite plates that are embedded within a matrix of retained austenite and a stress/strain induced transformation of the retained austenite phase into very hard untempered martensite. Phase transformation gives rise to work hardening, which is known as the transformation-induced plasticity effect [
2]. However, low transformation temperatures between 200 and 300 °C are required in order to obtain fine bainitic ferrite subunits [
3]. These steels contain high concentrations of carbon (close to 0.8%) and silicon (~1.5%) to ensure low transformation temperatures and a carbide-free bainitic microstructure [
4]. Rapid bainite transformation kinetics at temperatures, even below 200 °C, can be achieved by the introduction of nano-scale precipitates, which deplete the adjacent matrix of carbon and lead to the bainitic ferrite subunits nucleation [
3].
The increase in surface hardness due to stress/strain induced transformation under conditions of dry rolling and sliding in extremely fine pearlite steel, has been evaluated while using nano-indentation and can reach values of up to 750 HV [
5]. This also led to improved wear resistance, which was enhanced by reducing the distance between ferrite and cementite lamellas. Refined pearlite has a greater flow stress and work hardening rate, while finer cementite is able to accommodate more deformation prior to fracture [
6]. In this sense it is not important how the retained austenite was stabilized, due to the effect of Si or Al [
7], thermally [
8] or mechanically, provided the resulting toughness is sufficient to prevent the initiation and propagation of cracks from the surface. This was well illustrated in a study where the wear resistance of carbide free lower bainite, martensite, and pearlite in the same super bainite steel was practically the same [
9]. During abrasive wear, the retained austenite content of the austempered steel was reduced from an initial 44% to a final value of 12%, which is even lower than present after conventional quenching to martensite. On this example it was shown that a hard but brittle microstructure does not perform much better under abrasive conditions than a softer, but more ductile, one. Of course, depending on the hardness the wear mechanism will change accordingly. Therefore, it is important that the toughness of the material is sufficient for arresting crack propagation from the contact surface toward the bulk of the tool.
At the same hardness, the wear resistance of medium carbon steels has been reported to be up to 25% higher when treated into a carbide free bainitic microstructure as opposed to quenching and tempering into martensite. Furthermore, for carbide free bainitic medium carbon steels the surface hardness increased much more due to their higher work hardening capacity [
10]. In some cases, very high abrasive wear resistance is reported for low temperature carbide free bainitic steels, with their wear rate being as low as 1% of that exhibit by 100Cr6 steel, when heat treated to a needle-like lower bainite with hardness of about 60 HRC and the strength level of 2.3 GPa [
11]. This high abrasive wear resistance is largely attributed to the retained austenite content. However, while the retained austenite contributes to the steel wear resistance, its effect on toughness has been shown to be strongly deteriorating, when present in amounts that are close to or above 10% [
12]. Therefore, theoretically, it would be advantageous to locally introduce the retained austenite into the surface layer, while not compromising the toughness of the bulk material.
A method by which this could be accomplished is by the well-known phenomena of carbide dissolution under pressure. This effect has been documented in the field of bearing steels [
13]. During operation under heavy loads, the bearing steels undergo several microstructural changes, one of which is dislocation accumulation, particularly in heavily deformed regions. The accumulated dislocations shear carbide particles, which size is then reduced via dissolution, controlled by the migration of carbon from cementite towards dislocations. This requires a constant supply of carbon-unsaturated dislocations in the neighborhood of dissolving carbide particles. The dissolution tendency and rate are proportional to alloying elements content and dislocations density. Furthermore, smaller particles tend to dissolve much faster when compared to coarser ones, which can be intuitively explained in terms of a higher surface energy. However, there is also a threshold driving force value (12–15 kJ/mol), below which precipitates coarsening will occur rather than the dissolution [
13].
The aim of this research work was to investigate whether the effect of carbides dissolution under high pressure can be exploited under severe wear conditions, with the retained austenite only being generated in the vicinity of the hard abrading particles, such as oxide scale and hard wear particles, or more generally within regions of high contact pressure. Thus, increasing the wear resistance at the interface without compromising the toughness of the bulk material. Within a novel group of steel alloys termed kinetically activated bainite (KAB) steels, which have been introduced previously [
14], this concept enables the obtainment of very fine bainitic microstructures with a low retained austenite content. A KAB steel, which fulfils the above description, has been developed and its resistance to abrasive and adhesive wear evaluated and compared to conventional D2-type tool steel in the current work.
2. Materials and Methods
The material used in this work is new custom made high Si carbide-free bainitic cold work tool steel with the nominal chemical composition that is given in
Table 1. As a reference, commercial AISI D2 cold work tool steel has been used.
SIHARD S250 was cast in the form of 1 ton ingots, diffusion annealed at 1220 °C for 24 h, followed by hot rolling to the final shape of 62 mm × 32 mm flat profiles. Additionally, AISI D2 tool steel was cast in 1 ton ingot and then rolled to the same final dimension of 62 mm × 32 mm. Both of the steels were then soft annealed and test specimens machined from each steel.
As can be seen from the tempering diagram that is shown in
Figure 1, the hardness of SIHARD S250 steel (measured with Instron B2000 machine (Instron, Norwood, MA, USA), using Rockwell C method according to ASTM E18 standard [
15]) is continuously decreasing with increased tempering temperature, while a relatively high impact toughness (un-notched impact specimens; 7 mm × 10 mm × 55 mm) is obtainable within the desired working hardness range of 61–64 HRC, reached at low tempering temperatures. Furthermore, the tempering stability of SIHARD S250 is higher than for commercial AISI D2 steel, which can be explained by its high Si content.
The heat treatment conditions of the two investigated steels applied prior to testing are indicated with boxed X. The SIHARD S250 tool steel was quenched from 980 °C in oil and tempered once at 200 °C for 2 h to a hardness of 63 HRC and impact toughness of 50 J. On the other hand, AISI D2 was tempered twice at 520 °C, resulting in a similar hardness of about 62 HRC, but much lower toughness of only 15 J.
Compression tests were performed on standard short cylindrical test samples with a diameter of Φ13 mm and a length of 25 mm, according to the ASTM E9 standard [
16]. Testing was done with a force of 320 kN corresponding to a compressive stress of 2.4 GPa, which did not exceed the elastic limit of the steel.
The wear testing of the investigated tool steels in the final heat treated condition was performed under reciprocating dry sliding conditions at room temperature while using the ball-on-disc contact configuration. The abrasive wear mode was simulated by performing tests with Al2O3 ball (20 mm) sliding against polished tool steel disc (Ra = 0.10 µm) at a nominal contact pressure of 1.5 GPa (FN = 102 N) and an average sliding speeds of 0.01 (f = 1 Hz, stoke of 4 mm) and 0.12 m/s (f = 15 Hz, stroke of 4 mm), respectively. The wear volume of the removed tool steel material has been determined by three-dimensional (3D) profilometric analysis. On the other hand, adhesive wear determined as the volume of the counter-ball material adhered to the contact surface of the tool steel disc was simulated by performing sliding tests with a hardened 100Cr6 steel ball (20 mm, 58 HRC). In this case, tests were performed at a nominal contact pressure of 1 GPa (FN = 40 N) and sliding speed of 0.12 m/s. For all wear tests (abrasive and adhesive), the total sliding distance was 100 m.
The resulting abrasive wear volume and wear rate calculated as wear volume divided by normal load and sliding distance are the average of 10 sliding tests performed at two different sliding speeds and the adhesive wear rate the average of five sliding tests performed at single sliding speed of 0.12 m/s.
The galling resistance was examined by a load-scanning test [
17], where investigated tool steels were sliding against soft annealed S235J2 low carbon steel at a gradually increasing load. The tests were performed under dry sliding conditions and room temperature, sliding speed of 0.1 m/s, and load range of 100–1000 N. After the test critical loads for the beginning of low carbon steel transfer to the tool steel surface (L
C1) and transfer layer build-up (L
C2) were determined by microscopic analysis of the wear track.
Author Contributions
This article was conceptualized by B.P. and P.K., B.P. conducted the main investigation and wear resistance testing, B.P. and P.K. curated the data and prepared the original draft; Review and editing was conducted by B.P. and M.B. The work was completed under supervision of B.P., who also administrated the project and provided necessary resources. Authors contributed to the microstructural characterization in the following way: P.K. color metallography and stereo microscopy, M.B. FESEM Characterization. All authors have read and agreed to the published version of the manuscript.
Funding
The authors acknowledge the financial support from the Slovenian Research Agency (research core funding No. P2-0050).
Acknowledgments
The authors would like to express their sincere gratitude to Henrik Kaker for helpful discussions, help with SEM characterizations and XRD measurements. The authors also extend a special thanks to Darja Feispour, for her help with HRTEM characterization.
Conflicts of Interest
The authors declare no conflict of interest.
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