Microstructure and Hardness of Cold Work Vanadis 6 Steel after Subzero Treatment at −140°C

.e microstructure, phase constitution, and hardness of Cr-V ledeburitic tool steel Vanadis 6 subjected to subzero treatment at −140°C and for different soaking times have been investigated. .e light microscopy, scanning electron microscopy, and X-ray diffraction have been used for microstructural investigations. .e hardness has been evaluated by the Vickers method. .e 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..e 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..ismakes a serious support to the theory explaining the formation of “extra” carbides as a by-product 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.


Introduction
One of the major problems in heat treatment of high-carbon 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 (c 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 c 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 stress-induced c R transformation results in the formation of either the martensite or low bainite.erefore, 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 high-temperature 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 add-on step in the heat treatment of high-carbon high-alloyed 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.is 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 c R amount [1][2][3][4][5][6][7][8][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][12][13][14].(iv) SZT ledeburitic steels contain enhanced population density of small globular carbides (SGCs) [1-4, 8, 9, 14-19].e formation of these carbides is a result of more complete martensitic transformation as determined recently [14].
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.e 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].
e 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.
e current paper is focused on the investigations of microstructural alternations and their impact on resulting hardness of commercially available PM-manufactured cold work tool steel Vanadis 6, which was subjected to the subzero treatment at a temperature of −140 °C for different durations.e 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.
e steel was delivered in soft-annealed state (i.e., with ferrite-carbide microstructure), Figure 1, and its hardness was 284 HV 10. e 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.Advances in Materials Science and Engineering e 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].X-ray diffraction patterns were recorded using a Phillips PW 1710 device with filtered Co α1,2 characteristic radiation, in the range 45-130 °of the two-theta angle.e amount of retained austenite c R was determined according to the ASTM E975-13 standard [29].e 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.e austenite grain size G was determined by the Snyder-Graff method by the formula where S-G is the dimensionless Snyder-Graff intercept count number.

Results and Discussion
Figure 2 shows light micrograph of the examined steel after conventional quenching followed by SZT for 17 h.e microstructure consists of matrix and undissolved carbides, which are uniformly distributed throughout the material.
e matrix contains the martensite and retained austenite.e original austenitic grains are well visible.ey 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 e microstructure is composed of the matrix and three types of carbides, namely, the eutectic carbides (ECs), secondary carbides (SCs), and small globular carbides (SGCs).e population density of both the ECs and SCs is invariant over the heat treatment parameter range used.
is 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.e population density of SGCs increased with holding time at the temperature of SZT. is is clearly evident by comparing the microstructures in Figures 3(a)-3(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.
e formations of retained austenite are located in-between the martensitic domains.
e population density of SGCs as a function of the duration of SZT is shown in  e obtained results are in excellent agreement with those presented by other investigators for di erent Cr ledeburitic steels [2-4, 7, 18, 22].erefore, 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.e 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.
e c R amount decreases considerably with the application SZT, Table 1.In no-SZT samples, the amount of c R was 20.2 vol.%, and for SZT samples with 48 h holding time, it was just 3.24 vol.%.
e results of retained austenite amount measurements are consistent with those obtained by di erent researchers and for other Cr and Cr-V ledeburitic steels [3,4,7,9,22,31].ese researchers have reported that, for instance, the AISI D2 steel is almost free of c R after SZT performed at −196 °C for 36 h.Alternatively, Gavriljuk et al. [31] established that Cr-V ledeburitic steel X220 CrMoV 13-4 contained around 4% of retained austenite after long-term SZT at −196 °C.It is relevant to note that the c R always exists in the microstructure of high-carbon 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 c 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 c R more e ectively after longer processing times.ese results are counterintuitive on the rst sight because one can expect rather stronger e ect of lower processing temperature on the c R amount after short treatment too.Also, at least twice higher c R amounts in the specimens treated at −140 °C seem to be somewhat surprising since the processing temperature lies well below the characteristic martensite nish (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 di erence between the processing temperature and M f is much higher for the treatment in liquid nitrogen than in nitrogen gas at −140 °C.Lower c 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][32][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 c 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].
is 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 di erent 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.ese results are well   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 coe cient was calculated to be 0.858961.e correlation coe cient 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 high-carbon steels.is is due to very low martensite nish (M f ) temperature (it lies well below the room temperature in most cases) and also due to the positive volumetric e ect 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 e ort 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.is is an additional supporting fact to the theory, which was elaborated and demonstrated recently [14].
ese results infer that the as-quenched 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 e ect of SZT can be considered as minimal for durations of this treatment longer than 4 h.e enhancement of as-SZT bulk hardness of SZT steel over the CHT one can be simply referred to the reduction of soft-retained austenite and to the increased population density of small globular carbides.e current results can be considered to be in an excellent agreement with those reported for subzero-treated AISI D2 [2,3,21,34,35] and AISI D3 steel [4,18,36].

Conclusions
e Vanadis 6 ledeburitic tool steel has been austenitized, quenched, and subzero treated at a temperature of −140 °C for di erent durations.e obtained experimental results lead to following major conclusions: (1) e 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) e 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.e treatment at −140 °C leads to rather higher population density of these particles than the treatment at a temperature of boiling nitrogen.Advances in Materials Science and Engineering transformation, while the treatment at a temperature of boiling nitrogen leads to approx.half-fold retained austenite amount after long time treatment.(4) e as-quenched hardness of the Vanadis 6 tool steel manifests a moderate increase after SZT.(5) ere is a strong dependency of population density of SGCs and compressive stresses in the retained austenite.is fact supports the latest theory on the formation of enhanced population density of carbides, as a product of more complete martensitic transformation.

Figure 1 :
Figure 1: SEM micrograph showing the microstructure of the Vanadis 6 steel in as-delivered state.

2
)-3(d) show typical microstructures of the Vanadis 6 tool steel after CHT and after SZT at −140 °C for different durations.

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.e 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 CHTsamples and SZTsamples 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.e reference material treated at −196 °C had the maximum population density of SGCs of 193 × 10 3 /mm 2 for 24 h [19].

Figure 5 :
Figure 5: Population density of SGCs for samples processed by CHT and SZT, with various soaking times in nitrogen vapors at −140 °C.

Figure 4 :
Figure 4: Detail SEM micrograph showing the microstructure of Vanadis 6 steel after SZT at −140 °C for 24 h, with particular attention to the matrix microstructure.

Figure 7 :Figure 6 :
Figure 7: Bulk hardness HV 10 of the Vanadis 6 after SZT with di erent soaking times in nitrogen vapors.

Table 1 :
Amount of retained austenite (vol.%) in the SZT samples for various soaking times (h).