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Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering

Received: 4 August 2025     Accepted: 16 August 2025     Published: 3 December 2025
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Abstract

This article presents a comprehensive analysis of the structural and phase states, as well as the properties of plasma coatings on high-speed molybdenum steel after tempering. Advanced techniques, including scanning and transmission electron microscopy, X-ray diffractometry, and microcomposition analysis, were employed to investigate the impact of heat treatment on the microstructure and phase composition of the coating. Using methods of modern physical materials science, the structure, mechanical and tribological properties of the surface of a plasma deposited layer in a nitrogen medium with high-speed molybdenum steel on a substrate made of CSN 14331 medium carbon steel subjected to two times tempering at a temperature of 560-580°C for 1 hour have been studied. It was found that tempering of the deposited layer does not lead to a change in the morphology of the polycrystalline structure formed by eutectic grains and grains of a solid solution based on α-iron (BCC crystal lattice). The main phases are α-Fe (85% wt.) and carbides of complex composition Me23C6 (9% wt.) and Me6C (6% wt.), forming eutectic grains. The formation of nanoscale particles of iron and chromium carbides along the boundaries of martensite crystals formed during the transformation of residual austenite during tempering has been revealed. The hardness of the deposited layer is 4.3 times higher than the hardness of the substrate, the wear parameter is 1.5 * 10-6mm3/ N*m, and the coefficient of friction is 0.66.

Published in American Journal of Modern Physics (Volume 14, Issue 6)
DOI 10.11648/j.ajmp.20251406.11
Page(s) 234-243
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2025. Published by Science Publishing Group

Keywords

High-Speed Molybdenum Steel, Surfacing, Plasma Method, Heat Treatment, Elemental and Phase Composition, Defective Substructure, Hardness, Wear Resistance

1. Introduction
Over the past century, since the creation of the first high-speed steel P18, researchers have been actively developing new steels with wide limits of carbon content and alloying elements. The optimal composition of the created steels changes due to changes in the properties of the processed materials, technologies and designs of the production of products, the cost of alloying elements and many other factors. The subsequent tempering of high-speed steels of optimal composition is designed to enhance functional properties and provide high heat resistance due to the release of carbides Me2C and MC. Typically, in such steels (such as P6M5), the content of tungsten and molybdenum should be the same at a vanadium concentration of about 2%. Tungsten, molybdenum, and vanadium are distributed approximately equally in soluble and insoluble carbides. The first of them provide high hardness and heat resistance, while the second (insoluble) ones provide strength properties and toughness.
The main trends in the development of modern machine-building, metallurgical, and mining industries are characterized by the intensification of the use of materials with a unique combination of operational properties in structures and equipment parts, such as high abrasive, impact-abrasive, and waterjet wear resistance, and corrosion resistance . The premature failure of many parts is mainly due to processes occurring on the surface in the friction zone, as a result of which developments and research in the field of increasing the wear resistance of surface layers are relevant for advanced industries. One of the ways to increase the wear resistance of the surface of machine parts and mechanisms is to apply plasma coatings using modern surfacing materials for various operating conditions .
One of the fundamental tasks of modern physical materials science, which is of great practical importance, is to obtain coatings with high-speed steels with high performance properties that protect products from various types of wear, corrosion, dynamic loads and other external influences. The use of nitrogen as an alloying element in the formation of surfacing coatings, which leads to an increase in the microhardness of the structural components, significantly increases the operational properties . In recent years, scientific research and practical developments have been actively conducted in the field of energy- and resource-saving plasma surfacing technology with high-speed steels, which has significant advantages over other coating methods . Coatings with high-speed steels most fully meet modern industrial requirements in terms of both the level of achieved properties and economic efficiency.
Recent years have been marked by the increased use of high-speed steels with a molybdenum content of 8-10%. The replacement of W by Mo is due to a number of reasons. Previously, tungsten, which is an expensive and scarce strategic element, was widely used in the production of armor-piercing shells. Mo and W, located in the same group and neighboring periods of the Periodic Table of Elements, have a similar effect on the formation of the structural and phase state and properties of high-speed steels . However, despite this, the nature of transformations occurring in high-speed molybdenum steels and their properties may differ significantly from tungsten and tungsten-molybdenum ones .
Molybdenum steels have higher functional properties than tungsten or tungsten-molybdenum high-speed steels with a lower content of alloying elements, which is due to a number of reasons. Thus, the solubility of molybdenum in austenite of these steels is higher compared to tungsten and tungsten-molybdenum steels, which provides higher hardness values. During annealing and hot plastic deformation, smaller carbides are formed, which ensures the formation of a fine-grained structure and increased strength .
An additional improvement in the properties of surface layers formed by plasma surfacing with high-speed steels is achieved through the use of external energy effects by plasma, laser irradiation, and ion beams modifying the surface .
There practically have not been published any studies, either in Russia or abroad, based on highly informative methods of modern physical material science (and, first of all, electron microscopy) and devoted to the identification of the physical nature of structural and phase transformations of coatings of molybdenum high-speed steels during manufacture and subsequent heat treatment, which significantly reduces the prospects for practical elaboration.
In connection with the above, the purpose of the work was to study the fine structure and properties of the surface layer formed by plasma deposition of high-speed molybdenum steel on a medium-carbon steel substrate after high-temperature tempering.
2. Materials and Methods
Table 1. Modes of formation of the deposited layer of steel M9.

Welding current (A)

Arc voltage (V)

Welding speed (m/h)

Wire feed speed (m/h)

Arc length (mm)

145-150

50-55

18

60

20

A 4mm-diameter MoCrCoC system powder wire was used to form the deposited layer. Samples for research were obtained by plasma surfacing in nitrogen medium on CSN 14331 steel. The mode of formation of the deposited layer is shown in the Table 1. The surfacing was carried out in four layers with a total thickness of ~ 9-10 mm.
Chemical composition of CSN 14331 steel (weight. %): C - 0.3; Cr - 0.9; Мn - 0.8; Si - 0.9, the rest is Fe. The chemical composition of the deposited layer corresponds to steel M9 according to SAE-AISI M9 (T11309) Molybdenum High-Speed Steel (weight. %): Mo-8.85; Cr-3.57; Co-2.12; V-0.05; Si-1.12; Mn-0.56, Al-1.05, the rest - Fe. Superior grade argon (GOST 10157-79) with a flow rate of 6-8 liters/min was used as a plasma-forming gas; technically pure nitrogen (GOST 9293-74) with a flow rate of 20-22 liters/min was used as a protective gas. The plasma surfacing modes on the UD-417 installation did not differ from those described in the work.
The heat treatment of the deposited layer was carried out at a temperature of 560-580°C for 1 hour.
The phase composition of the deposited layer was studied by X-ray diffraction analysis. We used a DRON-8H X-ray diffractometer equipped with a parabolic mirror on the primary beam and a position-sensitive Mythen 2R 1D detector (640 channels, the size of one strip is 50 μ). The accelerating voltage applied to the X-ray tube was 40 kV, and the current was 20 mA. The shooting was carried out without rotating the sample. The shooting was carried out in the angular range of 2θ 35-95°. In all cases, the scan step was 0.1° and the exposure time was 15 seconds. Identification of the phase composition, qualitative and quantitative phase analysis, as well as refinement of the structure parameters were performed using the “CDA Crystallography and Diffraction Analysis” software package with a built-in powder standards file (JSC IC Burevestnik, version 2023-01-24-144022.8dec10c0f).
The structure and elemental composition of the deposited layer were studied by scanning electron microscopy (KYKY-EM6900 device with a thermionic tungsten cathode and an attachment for micro-X-ray spectral analysis of the elemental composition).
The defective substructure, elemental and phase composition of the deposited layer were studied by transmission electron diffraction microscopy of thin foils in the lumen mode and in the scanning mode (JEOL JEM-2100 device, Japan) . The method of microdiffraction analysis using the dark-field technique was used to analyze the phase composition of the material. Foils (objects studied by transmission electron diffraction microscopy) were produced by ion thinning (Ion Slicer EM-091001S installation, thinning is carried out by argon ions) of plates cut from massive samples on an Isomet Low Speed Saw installation parallel to the longitudinal axis of the sample, which made it possible to trace the change in the defective substructure of the material as it moved away from the fracture surface. Some of the foils were made by electrolytic polishing in a solution of chromium anhydride in orthophosphoric acid.
The hardness and Young’s modulus of the deposited layer were determined by Scanning Nano-Hardness Testers Nano Scan at an indenter load of 0.1 N. Studies of the tribological properties of the deposited layer according to the “pin-on-disc” scheme when sliding around a circle were performed on an Oscillating TRIBO tester (ASTM G99). Test conditions: a VK8 hard alloy ball with a diameter of 6 mm, a friction track radius of 2 mm, a counterbody distance of 100 m, a sample rotation speed of 25 mm/s, an indenter load of 5 N. Tribological tests were performed under dry friction conditions at room temperature. Tribotrek profiles were recorded on a contact profilometer (an Oscillating TRIBO tester attachment to the tribometer).
3. Results and Discussion
The profile of hardness and Young's modulus of the deposited layer subjected to additional tempering is shown in Figure 1. It is clearly seen that the hardness of the deposited material varies non-monotonously, reaching the highest value (16.1 GPa) in the surface layer; the average hardness of the deposited layer is 13.8 GPa. It should be noted that the hardness of the deposited layer before tempering reached a maximum value (14.1 GPa) also in the surface layer; the average hardness value for the thickness of the coating was 12.4 GPa. Thus, tempering of the deposited layer leads to an increase in the average hardness of the coating by 1.13 times. The average hardness of the substrate is 3.2 GPa and is significantly (4.3 times) lower than the average hardness of the deposited metal after tempering.
The Young's modulus is also maximal (269 GPa) in the surface layer of the surfacing and decreases slightly as it moves away from the surface of the deposited layer. The average value of the Young's modulus of the deposited layer after tempering is 262 GPa; before tempering, it is 234.9 GPa. Thus, tempering of the deposited layer leads to an increase in the average Young's modulus of deposition by 1.13 times.
Tribological tests have shown that the wear parameter of the deposited layer k = 1.5 * 10-6mm3/ N*m; the coefficient of friction of the material is μ = 0.66.
Figure 1. Hardness profile HIT (curve 1) and Young's modulus EIT (curve 2) of the deposited layer after tempering.
Tempering of the deposited layer does not lead to a change in the morphology of the surfacing structure at the macro level: a polycrystalline structure with eutectic layers along grain boundaries is revealed, which is traditional for high-speed steels . With large increases in the volume of grains, the etching structure is revealed, which obviously indicates the decomposition of the supersaturated solid solution of grains and the formation of nanoscale particles of the carbide phase.
The elemental composition of the deposited layer, studied by micro-X-ray spectral analysis, showed that in addition to the chemical elements of the wire used in the formation of the weld, oxygen atoms are present in the deposited layer, which indicates the oxidation of the material’s surface layer.
The mapping method visualized the distribution of the chemical elements of the deposited layer. The research results indicate an inhomogeneous distribution of molybdenum, chromium, aluminum, oxygen, and silicon in the deposited layer. Comparing the mutual distribution of aluminum, silicon, and oxygen atoms, we can assume the formation of aluminum and silicon oxides, as well as aluminosilicates, in the surface layer.
The "point-by-point" method was used to quantify the elemental composition of the characteristic morphological components of the deposited layer structure (rounded inclusions (indicated as "1" in Figure 2), interlayers along grain boundaries (indicated as "2" in Figure 2) and grain volume (indicated as "3" in Figure 2). Presented in Table 2 The results show that rounded inclusions are enriched with aluminum and oxygen atoms, which clearly indicates the formation of aluminum oxides in the deposited layer. The layers along the grain boundaries are mainly enriched with carbon, silicon, sulfur, vanadium, chromium, and molybdenum atoms, which may indicate a complex phase composition of these structural formations of the weld. The main chemical elements of the grain volume are carbon, chromium, iron and molybdenum.
Figure 2. The structure of the etched section of the surface of the deposited layer after tempering. The numbers indicate the surfaced elemental composition determination areas. Scanning electron microscopy.
Table 2. Results of X-ray spectral microanalysis of the surface layer, the image of the structure is shown in Figure 2.

Element

Point 1

Point 2

Point 3

From the area of Figure 2

wt. %

at. %

wt. %

at. %

wt. %

at. %

wt. %

at. %

C

0,0

0,0

7,08

26,74

7,64

26,9

0,0

0,0

O

41,35

55,69

2,01

5,69

1,91

5,05

2,16

7,27

Al

52,5

41,93

0,0

0,0

0,07

0,52

0,52

1,05

Si

0,0

0,0

1,38

2,23

1,09

1,63

1,15

2,21

S

0.0

0.0

1.21

1.72

0,0

0,0

0,0

0,0

V

0,0

0,0

0,31

0,27

0,0

0,0

0,07

0,08

Cr

0,33

0,14

5,18

4,52

3,14

2,55

3,64

3,78

Mn

0,0

0,0

0,0

0,0

0,0

0,0

0,58

0,57

Fe

5,82

2,24

57,97

47,08

80,51

60,96

80,54

77,87

Co

0,0

0,0

0,0

0,0

0,0

0,0

2,23

2,05

Mo

0,0

0,0

24,85

11,75

5,39

2,37

9,1

5,12

The phase composition of the deposited layer was studied by X-ray diffraction analysis. The results of the X-ray analysis presented in Table 3 indicate a significant transformation of the phase composition of the deposited layer after tempering. Firstly, residual austenite and Fe2C iron carbide are not detected. Secondly, the parameter of the α-phase crystal lattice decreases, which indicates the process of decomposition of a solid solution based on α-Fe. Thirdly, the size of the coherent scattering regions of the α-phase and Me6C carbide is significantly reduced, which may indicate the transformation of the defective substructure of the α-phase and the release of nanoscale particles of Me6C carbide.
Table 3. Calculated data obtained from radiographs of the deposited layer.

Phase

Phase fraction (wt. %)

Lattice parameters (Å)

OCD dimensions (nm)

Pre-tempering state

α-Fe

65

a = 2.887

52

γ-Fe

12

a = 3.598

34

М23C6

11

a = 10.466

23

Me6C

7

a = 11.002

28

Fe2C

5

a = 2.701

c = 4.449

13

Post-tempering state

α-Fe

85

a = 2.873

26

М23C6

9

a = 10.420

23

Me6C

6

a = 11.002

13

Studies of the elemental and phase composition, morphology of phases, and defective substructure of the deposited layer subjected to heat treatment performed by transmission electron microscopy showed that the grains have a lamellar structure characteristic of lamellar martensite of hardened steel (Figure 3). Along the grain boundaries, extended interlayers are observed with a structure characteristic of eutectic transformation, i.e. the eutectic of the lamellar type is located along the grain boundaries (Figure 3a). A dislocation substructure of the mesh type is observed in the volume of the plates. The scalar dislocation density, measured by the secant method , <p> = 6.5*1010 cm-2.
Figure 3. Electron microscopic image of the deposited layer structure: a - the image was obtained by STEM analysis methods; b - by TEM analysis methods.
Mapping methods have shown that the interlayers located along the grain boundaries are mainly enriched with molybdenum, chromium, carbon, and iron atoms. Eutectic grains are formed by alternating plates enriched mainly with iron and molybdenum atoms.
Figure 4. Results of a X-ray microanalysis of the deposited layer by the "point-by-point" method. The sites for determining the elemental composition are indicated.
By the method of "point by point" micro-X-ray spectral analysis, some clarifying quantitative studies of the eutectic and α-phase grains elemental composition were performed, see Figure 4 for electron microscopic image. It is clearly seen that the layered structure of the eutectic grain has a different elemental composition. The darker layers (spectra 1-3) are enriched with molybdenum and carbon atoms and do not contain aluminum atoms (Table 4). The light contrast layer (Spectrum 4) and the martensitic structure of the grain located next to the eutectic are enriched mainly with iron atoms. This suggests that the interlayers located along the grain boundaries are formed by alternating layers of carbides such as Me23C6 and Me6C and layers based on a solid iron solution.
Table 4. The results of the elemental analysis of the foil section shown in Figure 4.

Spectrum

Chemical element (at. %)

C

Al

Si

V

Cr

Mn

Fe

Mo

1

46.58

-0.01

2.43

0.17

2.57

0.39

19.79

28.08

2

53.43

0.03

2.32

0.08

2.22

0.09

15.91

25.92

3

30.28

0.03

2.19

0.41

3.46

0.18

23.22

40.23

4

25.56

0.13

1.44

-0.01

3.16

0.46

66.55

2.72

5

27.32

0.15

2.22

0.04

2.77

0.39

59.63

7.47

6

32.40

0.31

1.65

-0.03

3.02

0.29

57.27

5.09

7

32.74

0.59

2.49

-0.02

2.91

0.44

56.38

4.47

Figure 5. TEM image of the deposited layer structure: a - light field; b - microelectronogram; c, d - dark fields obtained in reflexes [112]α-Fe + [322]Fe3C (c) and [112]α-Fe + [631]Cr3C2 (d); on (b) the arrows indicate the reflexes in which dark fields are obtained: 1 - for (c); 2 - for (d). On (c, d), the arrows indicate the particles of the carbide phase.
Figure 6. TEM image of the structure of carbides and α-phase with microcracks: a - light field; b - microelectronogram; c, d - dark fields obtained in reflexes [002]α-Fe (c); [113]M6C (d); On (a) the arrows indicate a microcrack located along the interfaces of eutectic grains; on (b) the arrows indicate reflexes in which dark fields are obtained: 1 - for (c); 2 - (d); on (c), the arrows indicate the α-Fe sections, on (d), the arrows indicate the Me6C type carbide plates.
Figure 7. Electron microscopic image of the coating structure in the tempered state; a - bright field; b - microelectron diffraction pattern; c, d - dark fields obtained in reflections [244]M23C6 (c); [133]M23C6 (d); In (b), arrows indicate reflections in which dark fields were obtained: 1 - for (c); 2 - (d); in (c, d), arrows indicate microcracks located in the volume of carbide phase plates.
Studies of the phase composition of the deposited layer performed by transmission electron diffraction microscopy using microelectronogram analysis and dark-field analysis showed that the tempering of the deposited metal is accompanied by a partial transformation of residual austenite with the formation of iron carbide and chromium carbide particles along the boundaries of the martensite plates (Figure 5). No particles of the carbide phase were found in the volume of the martensite plates. No particles of the carbide phase were found in the volume of the martensite plates.
Above, it was shown that the surfacing under study is formed by grains of a solid solution based on α-Fe and grains of eutectic. Analysis of microelectronograms obtained from eutectic grains suggests that they are multiphase formations and are formed by layers of carbides of complex composition such as M23C6 or M6C (Figure 6d) and alpha-phase layers (Figure 6c). Along the interface Figure 6a) and in the volume Microcracks are detected in the plates of the carbide phase (Figure 7). This indicates that the eutectic grains are in an elastically stressed state and can be sources of macro cracks that can lead to the destruction of the deposited material.
4. Conclusions
The technology of plasma surfacing in a nitrogen medium of 4mm-diameter MoCrCoC system powder wire on steel CSN 14331 formed a surfaced layer with a thickness of ~ 10 mm. Argon of the highest grade was used as a plasma-forming gas. The deposited layer was tempered twice at a temperature of 560-580°C for 1 hour. Mechanical and tribological tests were performed and it was found that the hardness of the deposited layer is significantly (4.3 times) higher than the hardness of CSN 14331 steel, the wear parameter of the deposited layer k = 1.5 * 10-6mm3/ N*m; the coefficient of friction of the material μ = 0.66. It is shown that tempering of the deposited layer does not lead to a change in the morphology of the surfacing structure at the macro level: a polycrystalline structure formed by eutectic grains and grains of a solid solution based on α-iron (BCC crystal lattice) is revealed. The formation of a multiphase structure in the deposited layer was revealed, represented by an α-phase (solid solution based on the BCC crystal lattice Fe), a γ-phase (solid solution based on the FCC crystal lattice Fe), carbides of complex composition Me23C6 and Me6C, iron carbides of composition Fe3C and chromium of composition Cr3C2. The main phases are a solid solution based on α-Fe (85 wt. %) and carbides of complex composition Me23C6 (9 wt. %) and Me6C (6 wt. %), forming eutectic grains. It has been established that the tempering of the deposited layer is accompanied by the pre-transformation of residual austenite with the formation of nanoscale particles of iron and chromium carbides along the boundaries of martensite crystals. It can be assumed that the increase in hardness and wear resistance of the deposited metal as a result of heat treatment is due to the decomposition of a solid solution based on γ-iron with the formation of nanoscale inclusions of the carbide phase. Microcracks have been identified along the interfacial interfaces and in the volume of the plates of the carbide phase of eutectic grains, which can initiate the destruction of the deposited layer material under mechanical stress.
Abbreviations

TEM

Transmission Electron Microscopy

BCC

The Body-Centered Cubic

SEM

Scanning Electron Microscopy

Author Contributions
Irina Viktorovna
Yuriy Fedorovich Ivanov: Investigation, Methodology, Writing – original draft
Victor Evgenievich
Igor Yurievich Litovchenko: Visualization
Yuriy Sergeewich Serenkov: Writing - original draft
Alexander Sergeevich Chapaikin: Formal analysis
Funding
This work is supported by the Russian Science Foundation grant No. 23-19-00186, https://rscf.ru/project 23-19-00186
Conflicts of Interest
The authors declare no conflicts of interest.
References
[1] V. E. Gromov, A. S. Chapaykin, S. A. Nevsky, Structure, properties and models of high-speed steel surfacing after tempering and electron beam treatment, Polygraphist, Novokuznetsk, 2024, 171 p.
[2] A. S. Chaus, P. Pokorný, Ľ. Čaplovič, M. V. Sitkevich, J. Peterka, Complex fine-scale diffusion coating formed at low temperature on high-speed steel substrate, Appl. Surf. Sci. 437(2018) 257-270.
[3] J. Gerth, U. Wiklund, The influence of metallic interlayers on the adhesion of PVD TiN coatings on high-speed steel, Wear 264(2008) 885-892.
[4] N. Hashemi, A. Mertens, H.-M. Montrieux, J. T. Tchuindjang, O. Dedry, R. Carrus, J. Lecomte-Beckers, Oxidative wear behavior of laser clad high speed steel thick deposits: Influence of sliding speed, carbide type and morphology, Surf. Coat. Technol. 315(2017) 519-529.
[5] W. Darmawan, J. Quesada, R. Marchal, Characteristics of laser melted AISI-T1 high speed steel and its wear resistance, Surf. Eng. 23(2) (2007) 112-119.
[6] A. N. Emelyushin, E. V. Petrochenko, S. P. Nefediev, Inverstigation of the structure and impact-abrasive resistance of coatings of the Fe-C-Cr-Mn-Si system, additionally alloyed with nitrogen, Welding International 27(2) (2013) 150-153.
[7] S. P. Nefediev, A. N. Emelyushin, The influence of nitrogen on the formation of the structure and properties of plasma coatings of type 10P6M5, Bulletin of Yugorsky State University 3(62) (2021) 33-45.
[8] A. N. Emelyushin, E. V. Petrochenko, S. P. Nefediev, Investigation of the structure and impact-abrasive wear resistance of coatings of the Fe-C-Cr-Mn-Si system additionally alloyed with nitrogen, Welding Production 10(2011) 18-22.
[9] S. P. Nefediev, A. N. Emelyushin, Plasma surface hardening: monograph, TNT, Stary Oskol, 2021, 156 p.
[10] I. V. Mozgovoy, E. A. Shneider, Surfacing of high-speed steel, Publishing house of OmSTU, Omsk, 2016, 200 p.
[11] Yu. F. Ivanov, V. E. Gromov, A. I. Potekaev, T. P. Guseva, A. S. Chapaikin, E. S. Vashchuk, D. A. Romanov, Structure and properties of R18U surfacing of high-speed steel after its high tempering, Russian Physics Journal 66(7) (2023) 731-739.
[12] B. K. Rakhadilov, L. G. Zhurerova, M. Scheffler, A. K. Khassenov, Change in high temperature wear resistance of high speed steel by plasma nitriding, Bulletin of the Karaganda University. Physics Series 3(91) (2018) 59-65. EDN: KJWHYN.
[13] L. S. Kremnev, A. K. Onegina, L. A. Vinogradova, Features of transformations, structures and properties of molybdenum high-speed steels, Metallology and Heat Treatment of Metals 12(654) (2009) 13-19. EDN: KZSBKP.
[14] L. S. Kremnev, The theory of alloying and the creation of heat-resistant tool steels and alloys based on it, MiTOM 11(2008) 18-28. EDN: KVXKKF.
[15] I. K. Kupalova, Phase analysis and phase composition of high-speed steels (review), Factory Laboratory 1(1983) 27-40.
[16] Yu. F. Ivanov, Structural and phase transformations in a number of steels under static and dynamic heat treatment conditions. Abstract of the dissertation of Doctor of Physical and Mathematical Sciences, Moscow, 2002, 41 p.
[17] V. P. Rotstein, D. I. Proskurovsky, G. E. Ozur, Yu. F. Ivanov, Modification of the surface of metallic materials by low-energy high-current electron beams, SB RAS: Nauka, Novosibirsk, 2019, 348 p.
[18] N. N. Koval, Yu. F. Ivanov (Eds.), Evolution of the structure of the surface layer of steel subjected to electron-ion-plasma treatment, NTL, Tomsk, 2016, 298 p.
[19] J. Pout, G. Foti, D. Jacobson (Eds.), Modification and doping of the surface by laser, ion and electron beams, Mashinostroenie, Moscow, 1987, 424 p.
[20] A. G. Paikin, V. A. Shulov, V. I. Engelko, et al., Cratering on the surface of parts made of heat-resistant steel 15X16K5N2MVFAV-Sh when irradiated with high-current pulsed electron beams, Hardening Technologies and Coatings 10(2006) 9-14. EDN: HVMOZZ.
[21] V. A. Shulov, A. G. Paikin, A. B. Belov, et al., Modification of the surface of parts made of heat-resistant steels by high-current pulsed electron beams, Physics and Chemistry of Materials Processing 2(2005) 61-70. EDN: HSGMVF.
[22] F. R. Egerton, Physical Principles of Electron Microscopy, Springer International Publishing, Basel, 2016, 196 p.
[23] C. S. S. R. Kumar, Transmission Electron Microscopy. Characterization of Nanomaterials, Springer, New York, 2014, 717 p.
[24] C. B. Carter, D. B. Williams, Transmission Electron Microscopy, Springer International Publishing, Berlin, 2016, 518 p.
[25] L. M. Utevsky, Diffraction electron microscopy in metal science, Metallurgiya Publ., Moscow, 1973, 584 p.
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    Baklushina, I. V., Ivanov, Y. F., Gromov, V. E., Litovchenko, I. Y., Serenkov, Y. S., et al. (2025). Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering. American Journal of Modern Physics, 14(6), 234-243. https://doi.org/10.11648/j.ajmp.20251406.11

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    Baklushina, I. V.; Ivanov, Y. F.; Gromov, V. E.; Litovchenko, I. Y.; Serenkov, Y. S., et al. Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering. Am. J. Mod. Phys. 2025, 14(6), 234-243. doi: 10.11648/j.ajmp.20251406.11

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    Baklushina IV, Ivanov YF, Gromov VE, Litovchenko IY, Serenkov YS, et al. Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering. Am J Mod Phys. 2025;14(6):234-243. doi: 10.11648/j.ajmp.20251406.11

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  • @article{10.11648/j.ajmp.20251406.11,
      author = {Irina Viktorovna Baklushina and Yuriy Fedorovich Ivanov and Victor Evgenievich Gromov and Igor Yurievich Litovchenko and Yuriy Sergeewich Serenkov and Alexander Sergeevich Chapaikin},
      title = {Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering
    },
      journal = {American Journal of Modern Physics},
      volume = {14},
      number = {6},
      pages = {234-243},
      doi = {10.11648/j.ajmp.20251406.11},
      url = {https://doi.org/10.11648/j.ajmp.20251406.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20251406.11},
      abstract = {This article presents a comprehensive analysis of the structural and phase states, as well as the properties of plasma coatings on high-speed molybdenum steel after tempering. Advanced techniques, including scanning and transmission electron microscopy, X-ray diffractometry, and microcomposition analysis, were employed to investigate the impact of heat treatment on the microstructure and phase composition of the coating. Using methods of modern physical materials science, the structure, mechanical and tribological properties of the surface of a plasma deposited layer in a nitrogen medium with high-speed molybdenum steel on a substrate made of CSN 14331 medium carbon steel subjected to two times tempering at a temperature of 560-580°C for 1 hour have been studied. It was found that tempering of the deposited layer does not lead to a change in the morphology of the polycrystalline structure formed by eutectic grains and grains of a solid solution based on α-iron (BCC crystal lattice). The main phases are α-Fe (85% wt.) and carbides of complex composition Me23C6 (9% wt.) and Me6C (6% wt.), forming eutectic grains. The formation of nanoscale particles of iron and chromium carbides along the boundaries of martensite crystals formed during the transformation of residual austenite during tempering has been revealed. The hardness of the deposited layer is 4.3 times higher than the hardness of the substrate, the wear parameter is 1.5 * 10-6mm3/ N*m, and the coefficient of friction is 0.66.
    },
     year = {2025}
    }
    

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  • TY  - JOUR
    T1  - Structural and Phase States and Properties of Plasma Coating of High-Speed Molybdenum Steel After Tempering
    
    AU  - Irina Viktorovna Baklushina
    AU  - Yuriy Fedorovich Ivanov
    AU  - Victor Evgenievich Gromov
    AU  - Igor Yurievich Litovchenko
    AU  - Yuriy Sergeewich Serenkov
    AU  - Alexander Sergeevich Chapaikin
    Y1  - 2025/12/03
    PY  - 2025
    N1  - https://doi.org/10.11648/j.ajmp.20251406.11
    DO  - 10.11648/j.ajmp.20251406.11
    T2  - American Journal of Modern Physics
    JF  - American Journal of Modern Physics
    JO  - American Journal of Modern Physics
    SP  - 234
    EP  - 243
    PB  - Science Publishing Group
    SN  - 2326-8891
    UR  - https://doi.org/10.11648/j.ajmp.20251406.11
    AB  - This article presents a comprehensive analysis of the structural and phase states, as well as the properties of plasma coatings on high-speed molybdenum steel after tempering. Advanced techniques, including scanning and transmission electron microscopy, X-ray diffractometry, and microcomposition analysis, were employed to investigate the impact of heat treatment on the microstructure and phase composition of the coating. Using methods of modern physical materials science, the structure, mechanical and tribological properties of the surface of a plasma deposited layer in a nitrogen medium with high-speed molybdenum steel on a substrate made of CSN 14331 medium carbon steel subjected to two times tempering at a temperature of 560-580°C for 1 hour have been studied. It was found that tempering of the deposited layer does not lead to a change in the morphology of the polycrystalline structure formed by eutectic grains and grains of a solid solution based on α-iron (BCC crystal lattice). The main phases are α-Fe (85% wt.) and carbides of complex composition Me23C6 (9% wt.) and Me6C (6% wt.), forming eutectic grains. The formation of nanoscale particles of iron and chromium carbides along the boundaries of martensite crystals formed during the transformation of residual austenite during tempering has been revealed. The hardness of the deposited layer is 4.3 times higher than the hardness of the substrate, the wear parameter is 1.5 * 10-6mm3/ N*m, and the coefficient of friction is 0.66.
    
    VL  - 14
    IS  - 6
    ER  - 

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Author Information
  • Department of Natural Sciences, Siberian State Industrial University, Novokuznetsk, Russia

    Biography: Irina Viktorovna Baklushina is a researcher at Siberian State Industrial University, Novokuznetsk, Russia. She specializes in physical materials science, focusing on structural and phase states and the properties of plasma coatings and high-speed steels. Baklushina is an active author in the field of materials engineering with expertise in transmission electron microscopy and surface coating technologies. She has contributed to studies on plasma deposited layers and tempering effects on steels.

    Research Fields: Plasma coatings, High-speed steels, Materials characterization, Electron microscopy, Phase transformations

  • Laboratory of Plasma Emission Electronics, Institute of High-Current Electronics, Tomsk, Russia

    Biography: Yuriy Fedorovich Ivanov is a leading scientist at Siberian State Industrial University, Russia. He holds a doctorate in physics or materials science and focuses on microstructural analysis, phase transformations, and mechanical properties of steel alloys. Ivanov’s research involves heat treatment and plasma surfacing of high-speed steels. He has extensive experience in electron microscopy techniques and has published numerous papers on structural materials.

    Research Fields: Structural analysis of steels, Phase transformations, Electron microscopy, Plasma surface engineering, Tribological properties

  • Department of Natural Sciences, Siberian State Industrial University, Novokuznetsk, Russia

    Biography: Victor Evgenievich Gromov works at Siberian State Industrial University, Novokuznetsk. His research areas include metallurgical engineering, physical materials science, and phase transformations in high-speed steels. Gromov holds an advanced degree in materials science and collaborates closely with colleagues on the investigation of plasma coatings and structural analysis of alloys.

    Research Fields: Plasma surfacing, Microstructure of steels, Mechanical properties, Alloy phase composition, Materials science

  • Laboratory of Materials Science of Shape Memory Alloys, Institute of Strength Physics and Materials Science, Tomsk, Russia

    Biography: Igor Yurievich Litovchenko is affiliated with the Institute of Strength Physics and Materials Science, SB RAS, Tomsk, Russia. He is a specialist in electron microscopic visualization and materials characterization. His work involves detailed electron diffraction microscopy studies to analyze defective substructures and phase compositions of steel coatings. Litovchenko’s expertise supports structural metallurgy research on high-speed steels.

    Research Fields: Transmission electron microscopy, Phase analysis, Coating microstructure, Materials visualization, Nanostructured materials

  • Department of Natural Sciences, Siberian State Industrial University, Novokuznetsk, Russia

    Biography: Yuriy Sergeewich Serenkov is a research scientist at Siberian State Industrial University. His specialization includes surface engineering, plasma metallurgy, and materials characterization of steel coatings. Serenkov contributes to the development and analysis of plasma surfacing technologies and mechanical properties improvement

    Research Fields: Steel coatings, Surface modification, Microstructural characterization, Plasma engineering, Materials properties

  • Department of Natural Sciences, Siberian State Industrial University, Novokuznetsk, Russia

    Biography: Alexander Sergeevich Chapaikin is a materials science researcher based at Siberian State Industrial University. His research focuses on high-speed molybdenum steels, plasma coating technologies, and mechanical property enhancement through heat treatment processes. Chapaikin holds a relevant advanced degree and participates in studies on microstructural and phase transformation effects in steel

    Research Fields: High-speed steel alloys, Plasma deposited layers, Mechanical testing, Carbide phases, Steel surface engineering