Research Article  Open Access
Microstructure and Hardness of Cold Work Vanadis 6 Steel after Subzero Treatment at −140°C
Abstract
The microstructure, phase constitution, and hardness of CrV ledeburitic tool steel Vanadis 6 subjected to subzero treatment at −140°C and for different soaking times have been investigated. The light microscopy, scanning electron microscopy, and Xray diffraction have been used for microstructural investigations. The hardness has been evaluated by the Vickers method. The obtained results assist to draw that subzero treatment reduces the retained austenite amount and increases the population density of carbides, compared to conventional heat treatment. The extent of decrease in the retained austenite amount makes around 85%, and the increase in population density of small globular carbides was approximately fivefold. High compressive stresses were identified in the retained austenite, and their values follow the increase in carbide count. This makes a serious support to the theory explaining the formation of “extra” carbides as a byproduct of more complete martensitic transformation. As a result of the mentioned microstructural changes, the material hardness increased from 875 ± 16 HV 10 up to 954.6 ± 14 HV 10 for conventionally quenched and SZT steels, respectively.
1. Introduction
One of the major problems in heat treatment of highcarbon steels is too high amount of retained austenite, which appears in their microstructure after room temperature quenching. For example, Jurči et al. [1] reported that the amount of retained austenite (γ_{R}) in the ledeburitic tool steel Vanadis 6 was 20.2 ± 1.6 vol. % after room temperature quenching from the austenitizing temperature of 1050°C. Retained austenite is an undesirable microstructural feature as it is soft and metastable at low temperatures, and it is amenable to decompose when heavily loaded, for instance. Decomposition of the γ_{R} is always connected with dimensional changes, which can have detrimental effect on the durability of tools and precise parts. Also, an embrittlement of the materials can occur at these circumstances since the stressinduced γ_{R} transformation results in the formation of either the martensite or low bainite. Therefore, the retained austenite must be eliminated from the tools before use. One of the possible ways how the retained austenite can be removed is the application of hightemperature tempering. However, some steel grades cannot be tempered above a temperature of around 200°C, due to the risk of substantial hardness loss.
Subzero treatment (SZT) is an addon step in the heat treatment of highcarbon highalloyed steels where the materials are cooled down to temperatures well below the room temperature, held there for a predetermined duration, and reheated slowly to the room temperature. This kind of heat treatment leads to considerable alterations in the microstructure of steels, which can be summarized as follows:(i)SZT steels contain considerably reduced γ_{R} amount [1–9].(ii)As a result of both the extensive plastic deformation and spatial limitations, the martensite of SZT steels is clearly refined compared to that developed by room temperature quenching, and it contains enhanced number of lattice defects [1, 5, 10].(iii)In many cases, SZT steels contain precipitates of transient carbides after reheating to the room temperature as a result of accelerated precipitation rate caused by various metallurgical effects of SZT [11–14].(iv)SZT ledeburitic steels contain enhanced population density of small globular carbides (SGCs) [1–4, 8, 9, 14–19]. The formation of these carbides is a result of more complete martensitic transformation as determined recently [14].
Mentioned microstructural alterations are reflected in higher asSZT hardness [1–3, 11, 14, 15], better dimensional stability of components and tools [20, 21], and “extra” wear performance [2, 3, 9, 16, 22]. The toughness and fracture toughness are, however, worsened [23], except the cases where the steels are hightemperature tempered [24, 25].
Despite the basic metallurgical principles being responsible for alterations in the microstructure, mechanical properties and tribological performance are rather understood [14], the choice of “optimal” temperature of the SZT is still under debate.
In the middle of the 20th century, it was generally accepted that temperatures of approx. −79°C (−120°F) are sufficient to transform high portion of retained austenite into the martensite and thereby make beneficial effects like additional wear resistance, increased fatigue strength, and better aging stability of steels. Lower temperatures were not used for the SZT as the experiences of heat treaters indicated that there is a great risk of failure of tools, due to thermal shocks resulting from the immersion of tools into liquid nitrogen, for instance.
Only much later, a temperature of −196°C was suggested for treatment. Practical applications of tools have early shown that the treatment at the boiling temperature of liquid nitrogen further increases the wear resistance and hardness. Based on these facts, subzero treatment in liquid nitrogen became the standard processing route, and other temperatures did not have practical use in SZT. Also, the understanding of processes, which take place at cryotemperatures, has been realized by treatment of specimens at the temperature of −196°C.
Only few studies suggested other temperatures, for instance −140°C [11, 26] or, on the contrary, a temperature of liquid helium [11, 27] for the treatment of Cr ledeburitic tool steels. The obtained experimental results indicate that some processes, which are responsible for the abovementioned ameliorations in properties, may proceed faster at −140°C than at −196°C; thus, this schedule might bring some benefits into the SZT. Alternatively, the use of the temperature of boiling helium (−269°C, 4.2 K) can provide an “extra” driving force for the martensitic transformation and thereby for the formation of SGCs also. However, it is inevitable that treatment times would be very long as there is little atomic movement at such a low temperature [11].
The main goal of the current experimental works is then to make a comprehensive study on what happens in ledeburitic steels when they are subjected to the SZT at −140°C. The current paper is focused on the investigations of microstructural alternations and their impact on resulting hardness of commercially available PMmanufactured cold work tool steel Vanadis 6, which was subjected to the subzero treatment at a temperature of −140°C for different durations. The same steel processed by room temperature quenching as well as the samples after subzero treatment at −196°C has been used as the reference material.
2. Experimental
The experimental material was the tool steel Vanadis 6 with nominally 2.1% C, 1.0% Si, 0.4% Mn, 6.8% Cr, 1.5% Mo, and 5.4% V and Fe as balance, made by PM. The steel was delivered in softannealed state (i.e., with ferritecarbide microstructure), Figure 1, and its hardness was 284 HV 10. The carbides are distributed uniformly within the matrix, with no preferential orientation.
Samples for the microstructural investigations were cylinders with a diameter of 17 mm and height of 6 mm. Conventional heat treatment (CHT) consisted of the following steps: heating up to the austenitizing temperature of 1050°C in a vacuum furnace, holding at the temperature for 30 min, and nitrogen gas quenching (5 bar). SZT has been completed at a temperature of −140°C and for 4, 10, 17, 24, 36, and 48 h. No tempering of the steel was carried out in order to highlight the microstructural changes due to the SZT itself.
Metallographic samples were prepared by standard preparation line and etched with the Villela–Bain reagent for the light microscopy or with picric acid for the SEM observation.
The microstructure was recorded using the light microscope NEOPHOT 32 and the scanning electron microscope JEOL JSM 7600 F device equipped with an EDS detector (Oxford Instruments), at an acceleration voltage of 15 kV. For each duration of subzero treatment, quantitative analysis of carbides has been done on twenty randomly acquired SEM micrographs. For details of the categorization of the carbides, check [1, 28]. Xray diffraction patterns were recorded using a Phillips PW 1710 device with filtered Co_{α1,2} characteristic radiation, in the range 45–130° of the twotheta angle. The amount of retained austenite γ_{R} was determined according to the ASTM E97513 standard [29]. The stress values in the retained austenite have been calculated from the lattice deformation (true strain), assuming pure elastic deformation (validity of Hook’s law), and considering the Young modulus to be 225 GPa [30].
Macrohardness measurements were completed by the Vickers (HV 10) method. Each metallographic specimen was measured 5 times, and the mean value and standard deviation from the measurements were calculated. The austenite grain size G was determined by the Snyder–Graff method by the formulawhere SG is the dimensionless Snyder–Graff intercept count number.
3. Results and Discussion
Figure 2 shows light micrograph of the examined steel after conventional quenching followed by SZT for 17 h. The microstructure consists of matrix and undissolved carbides, which are uniformly distributed throughout the material. The matrix contains the martensite and retained austenite. The original austenitic grains are well visible. They are very fine—the grain size was determined to be 10.26 ± 0.14 according to the Snyder–Graff method.
SEM micrographs, Figures 3(a)–3(d) show typical microstructures of the Vanadis 6 tool steel after CHT and after SZT at −140°C for different durations. The microstructure is composed of the matrix and three types of carbides, namely, the eutectic carbides (ECs), secondary carbides (SCs), and small globular carbides (SGCs). The population density of both the ECs and SCs is invariant over the heat treatment parameter range used. This is because the ECs do not undergo the dissolution during austenitizing, and the level of dissolution of the SCs is constant at fixed austenitizing temperature. The population density of SGCs increased with holding time at the temperature of SZT. This is clearly evident by comparing the microstructures in Figures 3(a)–3(d).
(a)
(b)
(c)
(d)
Detail SEM micrograph acquired at high magnification, Figure 4, demonstrates that the matrix is composed of the martensite and small amount of the retained austenite. The formations of retained austenite are located inbetween the martensitic domains.
The population density of SGCs as a function of the duration of SZT is shown in Figure 5. It is obvious that the population density of SGCs increased very rapidly up to 24 h of soaking time and then rather slightly decreased. The mean values of population density of SGCs were 48 × 10^{3}, 176 × 10^{3}, 179 × 10^{3}, 198 × 10^{3}, 209 × 10^{3}, 193 × 10^{3}, and 183 × 10^{3}/mm^{2} for CHT samples and SZT samples for 4, 10, 17, 24, 36, and 48 h, respectively. Here, it should be noted that the values, with respect to the statistical uncertainty at a level of 95%, considerably overlap for the samples treated for 4 and 10 h. It is shown that the maximum population density of SGCs was achieved for 24 h storage time at −140°C. The reference material treated at −196°C had the maximum population density of SGCs of 193 × 10^{3}/mm^{2} for 24 h [19].
The obtained results are in excellent agreement with those presented by other investigators for different Cr ledeburitic steels [2–4, 7, 18, 22]. Therefore, one can suggest that the fact that the SZT produces enhanced number and population density of these particles is generally a valid phenomenon for the ledeburitic cold work tool steels. In the recent two papers [14, 19], it has been demonstrated that the SZT at −196°C increases the population density of SGCs in the Vanadis 6 steel. The values of population density were 169 × 10^{3}, 188 × 10^{3}, 193 × 10^{3}, and 160 × 10^{3}/mm^{2} for the material subzero treated for 10, 17, 24, and 48 h, respectively. By comparing the results obtained by two SZT temperatures, it is evident that the SZT at −140°C produces rather higher population density of SGCs.
The γ_{R} amount decreases considerably with the application SZT, Table 1. In noSZT samples, the amount of γ_{R} was 20.2 vol. %, and for SZT samples with 48 h holding time, it was just 3.24 vol. %.

The results of retained austenite amount measurements are consistent with those obtained by different researchers and for other Cr and CrV ledeburitic steels [3, 4, 7, 9, 22, 31]. These researchers have reported that, for instance, the AISI D2 steel is almost free of γ_{R} after SZT performed at −196°C for 36 h. Alternatively, Gavriljuk et al. [31] established that CrV ledeburitic steel X220 CrMoV 134 contained around 4% of retained austenite after longterm SZT at −196°C. It is relevant to note that the γ_{R} always exists in the microstructure of highcarbon highalloyed ledeburitic steels in their untempered state because the martensitic transformation is never completed in these materials.
In recent studies, it has been reported that the SZT in liquid nitrogen (−196°C) carried out for 4, 10, 17, 24, and 48 h reduces the retained austenite amount to 9.9 ± 1.6, 2.9 ± 0.6, 2.1 ± 0.5, 2.9 ± 0.6, and 3.0 ± 0.7 vol. %, respectively [1, 14, 19]. It is seen that the γ_{R} amount is considerably lower for the specimens processed at −140°C than that after processing at −196°C for short time treatments but the treatments in liquid nitrogen remove the γ_{R} more effectively after longer processing times. These results are counterintuitive on the first sight because one can expect rather stronger effect of lower processing temperature on the γ_{R} amount after short treatment too. Also, at least twice higher γ_{R} amounts in the specimens treated at −140°C seem to be somewhat surprising since the processing temperature lies well below the characteristic martensite finish (M_{f}) temperature (−69°C). However, it should be noticed that there is much higher driving force for the martensitic transformation at −196°C, that is, the temperature difference between the processing temperature and M_{f} is much higher for the treatment in liquid nitrogen than in nitrogen gas at −140°C. Lower γ_{R} amount after short time treatment at −140°C, on the contrary, can be explained by the following consideration: Isothermal martensitic transformation, which proceeds during the hold at the lowest processing temperature, is connected with plastic deformation of freshly formed martensite, as demonstrated in [31–33]. It is logical to expect that plastic deformation proceeds faster at −140°C than at −196°C, and this can act in favour of more pronounced γ_{R} reduction in the early stage of isothermal martensitic transformation.
By comparing the data in Table 1 and the obtained results of population density of SGCs, Figure 5, it is obvious that there is close relation between these two microstructural parameters. Similar results were reported for the same material after subzero treatment in liquid nitrogen [1, 14]. This indicates that there exists a general validity of the relation “the less the retained austenite is, the higher the population density of SGCs is.” In other words, enhanced population density of SGCs can be attributed to more complete martensitic transformation.
Table 2 shows calculated hydrostatic stresses in the retained austenite for different SZT samples. It is shown that the compressive stresses in the retained austenite exceed 1000 MPa and that the highest stresses were developed in the material that was SZT for 24 h. These results are well consistent with the obtained results by Villa et al. [10] who reported on high compressive stresses in the retained austenite of 100Cr6 ball bearing steel after application of SZT. Figure 6 shows the dependence of both the population density of SGCs and compressive stress in austenite on the duration of SZT. For these two curves, the correlation coefficient was calculated to be 0.858961. The correlation coefficient is greater than 0.8; hence, there is a strong dependency of these parameters.

At this place, it is noteworthy once again to pay attention to the presence of considerably enhanced population density of SGCs: As well known, the martensitic transformation is never completed in highcarbon steels. This is due to very low martensite finish (M_{f}) temperature (it lies well below the room temperature in most cases) and also due to the positive volumetric effect of the transformation. As a result, compressive stresses are built up in the austenite, which hinder further progress in the transformation. In SZT, however, the temperature lies well below the M_{f}, and this makes a strong driving force for continuing of the transformation. As discussed and explained recently [14], the SGCs are a byproduct of the martensitic transformation that takes place at cryotemperatures and resulted from the effort of the material to relax the stresses and thereby enabling the further martensitic transformation. In the present study, close correlation between the compressive stress in the retained austenite and the population density of SGCs has been established. This is an additional supporting fact to the theory, which was elaborated and demonstrated recently [14].
The bulk hardness of SZT Vanadis 6 tool steel is shown in Figure 7. The hardness of CHT steel was 875 ± 16 HV 10. The hardness of the SZT steel soaked in nitrogen vapor for 4, 10, 17, 24, 36, and 48 h were 949 ± 13.5, 949.2 ± 15.6, 933.2 ± 16.8, 925.2 ± 13.3, 940.8 ± 6.4, and 954.6 ± 14 HV 10, respectively. These results infer that the asquenched bulk hardness of Vanadis 6 steel is improved due to SZT, whereas the improvement is almost independent on the duration of subzero treatment at −140°C. In other words, this kind of treatment increases the hardness compared to the state after CHT, but the effect of SZT can be considered as minimal for durations of this treatment longer than 4 h.
The enhancement of asSZT bulk hardness of SZT steel over the CHT one can be simply referred to the reduction of softretained austenite and to the increased population density of small globular carbides. The current results can be considered to be in an excellent agreement with those reported for subzerotreated AISI D2 [2, 3, 21, 34, 35] and AISI D3 steel [4, 18, 36].
4. Conclusions
The Vanadis 6 ledeburitic tool steel has been austenitized, quenched, and subzero treated at a temperature of −140°C for different durations. The obtained experimental results lead to following major conclusions:(1)The Vanadis 6 tool steel is composed of the matrix (the martensite and the retained austenite), ECs, SCs, and SGCs (with a size up to 500 nm, mostly around 100 nm).(2)The population density of small globular carbides is several times increased due to the SZT, with a maximum after SZT realized for a soaking time of 24 h. The treatment at −140°C leads to rather higher population density of these particles than the treatment at a temperature of boiling nitrogen.(3)The application of SZT reduces the amount of retained austenite in Vanadis 6 tool steel considerably. Moreover, it has been found that the treatment at −140°C acts more effectively in reduction of retained austenite in early stages of isothermal γ to α′ transformation, while the treatment at a temperature of boiling nitrogen leads to approx. halffold retained austenite amount after long time treatment.(4)The asquenched hardness of the Vanadis 6 tool steel manifests a moderate increase after SZT.(5)There is a strong dependency of population density of SGCs and compressive stresses in the retained austenite. This fact supports the latest theory on the formation of enhanced population density of carbides, as a product of more complete martensitic transformation.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
The authors acknowledge that this paper is a result of experiments realized within the project VEGA 1/0264/17. In addition, this publication is the result of the project implementation “Centre for Development and Application of Advanced Diagnostic Methods in Processing of Metallic and NonMetallic Materials–APRODIMET,” ITMS: 26220120014, supported by the Research & Development Operational Programme funded by the ERDF.
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Copyright © 2018 Juraj Ďurica et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.