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Journal articles on the topic 'Vacuum-arc evaporation'

Author: Grafiati

Published: 28 May 2022

Last updated: 31 July 2025

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1

Proskurovsky, Dmitry I., Sergey A. Popov, Andrey V. Kozyrev, Elena L. Pryadko, Alexander V. Batrakov, and Alexander N. Shishkov. "Droplets Evaporation in Vacuum Arc Plasma." IEEE Transactions on Plasma Science 35, no. 4 (2007): 980–85. http://dx.doi.org/10.1109/tps.2007.897906.

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2

CHAYAHARA, Akiyoshi, Yoshiaki MOKUNO, Nobuteru TSUBOUCHI, Yuji HORINO, Atsushi KINOMURA, and Kanenaga FUJII. "Coaxial Evaporation Source Using Vacuum Arc Discharge." SHINKU 40, no. 3 (1997): 300–302. http://dx.doi.org/10.3131/jvsj.40.300.

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3

Shiina, Kentaro, and Shinichi Sasayama. "Manganese evaporation during vacuum arc furnace remelting." DENKI-SEIKO[ELECTRIC FURNACE STEEL] 56, no. 1 (1985): 23–29. http://dx.doi.org/10.4262/denkiseiko.56.23.

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4

Brzezinka, Tomasz L., Jeff Rao, Jose M. Paiva, et al. "Facilitating TiB2 for Filtered Vacuum Cathodic Arc Evaporation." Coatings 10, no. 3 (2020): 244. http://dx.doi.org/10.3390/coatings10030244.

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TiB2 is well established as a superhard coating with a high melting point and a low coefficient of friction. The brittle nature of borides means they cannot be utilised with arc evaporation, which is commonly used for the synthesis of hard coatings as it provides a high deposition rate, fully ionised plasma and good adhesion. In this work, TiB2 conical cathodes with non-standard sintering additives (carbon and TiSi2) were produced, and the properties of the base material, such as grain structure, hardness, electrical resistivity and composition, were compared to those of monolithic TiB2. The d

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5

Сысоев, Юрий Александрович. "ПРО МОЖЛИВІСТЬ УСУНЕННЯ КРАПЕЛЬНОЇ ФАЗИ ВАКУУМНО-ДУГОВОГО РОЗРЯДУ ВВЕДЕННЯМ ЕНЕРГІЇ У ЗОНУ ЇЇ ТРАНСПОРТУВАННЯ". Aerospace Technic and Technology, № 2 (25 березня 2017): 71–77. http://dx.doi.org/10.32620/aktt.2017.2.08.

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Briefly reviewed the known methods of reducing the amount of microdroplets in a vacuum arc coatings. It has been shown that they do not allow to completely eliminate the microdroplets of the plasma stream. The possibility of removing the drip phase vacuum arc discharge by evaporation it when entering the microwave energy in its transportation zone was considered. Vacuum arc apparatus for implementing this method was proposed. The estimation of microwave energy required to evaporate droplets of titanium at a current of arc 100 A was done. Unaccounted the factors that can lead to lower of obtain

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6

Scheibe, H. J., and P. Siemroth. "Film deposition by laser-induced vacuum arc evaporation." IEEE Transactions on Plasma Science 18, no. 6 (1990): 917–22. http://dx.doi.org/10.1109/27.61503.

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7

Vetter, J., O. Knotek, J. Brand, and W. Beele. "MCrAlY coatings deposited by cathodic vacuum arc evaporation." Surface and Coatings Technology 68-69 (December 1994): 27–31. http://dx.doi.org/10.1016/0257-8972(94)90133-3.

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8

Ellrodt, M., and H. Mecke. "Possibilities of influencing vacuum arc evaporation by time-dependent arc current." Surface and Coatings Technology 74-75 (September 1995): 241–45. http://dx.doi.org/10.1016/0257-8972(95)08345-6.

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9

ZHANG, Zhefeng, Lijun WANG, Ze YANG, Ming LUO, and Jiagang LI. "Numerical simulation of low-current vacuum arc jet considering anode evaporation in different axial magnetic fields." Plasma Science and Technology 24, no. 4 (2022): 044002. http://dx.doi.org/10.1088/2058-6272/ac3903.

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Abstract As the main source of the vacuum arc plasma, cathode spots (CSs) play an important role on the behaviors of the vacuum arc. Their characteristics are affected by many factors, especially by the magnetic field. In this paper, the characteristics of the plasma jet from a single CS in vacuum arc under external axial magnetic field (AMF) are studied. A multi-species magneto-hydro-dynamic (MHD) model is established to describe the vacuum arc. The anode temperature is calculated by the anode activity model based on the energy flux obtained from the MHD model. The simulation results indicate

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10

Taran, A., O. Kyslytsyn, O. Podshyvalova, S. Taran, and A. Okhrimovskyy. "Thermal vacuum evaporation peculiarities of perovskite-type barium-strontium hafnate." Journal of Physics: Conference Series 2628, no. 1 (2023): 012031. http://dx.doi.org/10.1088/1742-6596/2628/1/012031.

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Abstract Experimental results are presented on the thermal vacuum evaporation of barium hafnate BaHfO3 and double barium-strontium hafnate Ba0.5Sr0.5HfO3, which are included together with finely dispersed tungsten as components in sintered composites. It is found that at T = 1900 K only barium and barium oxide are the products of BaHfO3 evaporation, i.e., congruent evaporation of BaHfO3 does not occur. Investigations of Ba0.5Sr0.5HfO3 evaporation at T = 1600 K showed that it also does not evaporate congruently. At the same time, the nucleation of a new phase of BaO·SrO in the form of structure

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11

Duan, Xingkai, Junyou Yang, Wei Zhong, Wei Zhu, Siqian Bao, and Xi'an Fan. "Synthesis of Bi2Te3 nanopowders by vacuum arc plasma evaporation." Powder Technology 172, no. 2 (2007): 63–66. http://dx.doi.org/10.1016/j.powtec.2006.10.009.

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12

Siemroth, Peter, Otmar Zimmer, Thomas Schülke, and Jörg Vetter. "Vacuum arc evaporation with programable erosion and deposition profile." Surface and Coatings Technology 94-95 (October 1997): 592–96. http://dx.doi.org/10.1016/s0257-8972(97)00502-1.

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13

Duan, X. K., and Y. Z. Jiang. "Synthesis of Sb2Te3 nanopowders by vacuum arc plasma evaporation." Vacuum 85, no. 11 (2011): 1052–54. http://dx.doi.org/10.1016/j.vacuum.2011.03.021.

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14

Vetter, J., H. J. Scholl, and O. Knotek. "(TiCr)N coatings deposited by cathodic vacuum arc evaporation." Surface and Coatings Technology 74-75 (September 1995): 286–91. http://dx.doi.org/10.1016/0257-8972(95)08350-2.

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15

Fedorov L. Yu., Ushakov A. V., and Karpov I. V. "Synthesis and chemoresistive sensitivity to hydrogen of nanostructured CuO films." Technical Physics Letters 48, no. 7 (2022): 58. http://dx.doi.org/10.21883/tpl.2022.07.54041.19197.

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Highly porous CuO films up to 1 μm thick consisting of vertically oriented nanowires ~ 50 nm in diameter were synthesized by copper evaporation in a vacuum arc discharge in an argon/oxygen atmosphere followed by deposition on heated substrates. The phase composition and polycrystalline nature of the films were confirmed by X-ray diffraction. On the example of gaseous hydrogen H2 at a sensor operating temperature of 300oC, sensory characteristics of CuO films were studied. The qualitative mechanism of the effect of gas on the electrical characteristics of the nanostructured CuO film is describe

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16

Dorraki, Naghme, Ralf Methling, and Sergey Gortschakow. "Optical Diagnostics of Anode Surface Temperature in Vacuum Interrupters with Different CuCr Compositions." PLASMA PHYSICS AND TECHNOLOGY 10, no. 1 (2023): 28–31. http://dx.doi.org/10.14311/ppt.2023.1.28.

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The requirements for contact material in vacuum interrupters are demanding because the arc medium is formed by electrode evaporation during the operation. Copper chromium alloy (CuCr) is widely used as contact material. Different compositions could result in a different rate of successful interruption. This work compares vacuum arc properties for two CuCr compositions - 75/25 and 50/50 weight percent. The contact surface temperature is measured during and after the vacuum arc with an AC current flow at 2kA magnitude. Quantitative characterization of the contact surface temperature was obtained

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17

Huang, Xiaolong, Shangyu Yang, Zhiyun Wu, et al. "Investigation of the spatial distribution characteristics of multiple species in a vacuum arc." Physics of Plasmas 30, no. 3 (2023): 033903. http://dx.doi.org/10.1063/5.0127802.

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The spatial distribution of multiple species in a vacuum arc is an essential microscopic feature. Ionization, recombination, and species diffusion are the main factors affecting the distribution of arc particles. The purpose of this paper is to investigate the spatial distribution characteristics of multiple species in a vacuum arc using a high-speed camera and interference filters. CuCr50 and pure copper plate electrodes were used to conduct arc-burning experiments in a demountable vacuum chamber. The distribution of different species was obtained by arranging interference filters outside the

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18

Elstner, F., C. Gautier, O. Piot, et al. "Comparative Study of the Stress in Chromium Films Deposited by Vacuum Arc Evaporation, Vacuum Evaporation, and DC Magnetron Sputtering." Physica Status Solidi (a) 154, no. 2 (1996): 669–79. http://dx.doi.org/10.1002/pssa.2211540220.

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19

Journal, Baghdad Science. "Study the influence of Annealing upon electrical properties of The prepared films ZnSe by Thermal evaporation in Vacuum." Baghdad Science Journal 1, no. 2 (2004): 253–57. http://dx.doi.org/10.21123/bsj.1.2.253-257.

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Thin films of ZnSe arc deposited on glass substrates by thermal evaporation in vacuum with different thickness (1000, 2700, 4000) A° temperature (293-373) °K are studies the electrical properties before and after annealing. The result show decrease D.0 conductivity and increasing the activation energy Eat.

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20

Yamamoto, Shinji, and Toru Iwao. "Evaporation Rate of Vacuum Arc Cathode Spot Affected by Ambient Pressure." IEEJ Transactions on Power and Energy 136, no. 3 (2016): 311–17. http://dx.doi.org/10.1541/ieejpes.136.311.

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21

Dukhopel’nikov, D. V., D. V. Kirillov, and V. S. Bulychev. "Characteristics of silicon microdroplets in coatings deposited by vacuum arc evaporation." Polymer Science Series D 9, no. 2 (2016): 238–42. http://dx.doi.org/10.1134/s1995421216020040.

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22

Dukhopelnikov, D. V., and D. V. Kirillov. "Evaporation of polycrystalline silica-aluminium cathode in cathodic arc vacuum discharge." Izvestiya vysshikh uchebnykh zavedenii. Fizika, no. 11 (2019): 68–74. http://dx.doi.org/10.17223/00213411/62/11/68.

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23

Ushakov, A. V., I. V. Karpov, L. Yu Fedorov, et al. "Synthesis of Quasicrysalline Powders and Coatings by Vacuum Arc Plasma Evaporation." Physics of the Solid State 61, no. 12 (2019): 2547–52. http://dx.doi.org/10.1134/s1063783419120576.

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24

Minami, Tadatsugu, Satoshi Ida, Toshihiro Miyata, and Youhei Minamino. "Transparent conducting ZnO thin films deposited by vacuum arc plasma evaporation." Thin Solid Films 445, no. 2 (2003): 268–73. http://dx.doi.org/10.1016/s0040-6090(03)01159-3.

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25

Miyata, Toshihiro, Satoshi Tsukada, and Tadatsugu Minami. "Preparation of anatase TiO2 thin films by vacuum arc plasma evaporation." Thin Solid Films 496, no. 1 (2006): 136–40. http://dx.doi.org/10.1016/j.tsf.2005.08.294.

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26

Kim, Il Ho, Jung Il Lee, Soon Chul Ur, Kyung Wook Jang, Good Sun Choi, and Joon Soo Kim. "Annealing Effect on the Thermoelectric Properties of Undoped CoSb₃." Solid State Phenomena 118 (December 2006): 565–70. http://dx.doi.org/10.4028/www.scientific.net/ssp.118.565.

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Binary skutterudite CoSb3 compounds were prepared by the arc melting and hot pressing processes and their thermoelectric properties were investigated at 300K-600K. Annealing effect was examined and it was correlated to phase transformation and homogenization. Thermoelectric properties of the arc-melted and hot-pressed CoSb3 were discussed and compared. Undoped CoSb3 prepared by the arc melting showed p-type conduction and metallic behavior at all temperatures examined. However, hot pressed specimens showed n-type conduction, possibly due to Sb evaporation. Thermoelectric properties were remark

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27

Qu, Shuai-Jie, Shu-Qi Huang, Chao-Qian Guo, et al. "Chromium arc plasma characterization, structure and properties of CrN coatings prepared by vacuum arc evaporation." Vacuum 209 (March 2023): 111796. http://dx.doi.org/10.1016/j.vacuum.2022.111796.

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28

Wan, L., and R. F. Egerton. "Preparation and characterization of thin films of carbon nitride." Proceedings, annual meeting, Electron Microscopy Society of America 53 (August 13, 1995): 104–5. http://dx.doi.org/10.1017/s0424820100136891.

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INTRODUCTION Recently, a new compound carbon nitride (CNx) has captured the attention of materials scientists, resulting from the prediction of a metastable crystal structure β-C3N4. Calculations showed that the mechanical properties of β-C3N4 are close to those of diamond. Various methods, including high pressure synthesis, ion beam deposition, chemical vapor deposition, plasma enhanced evaporation, and reactive sputtering, have been used in an attempt to make this compound. In this paper, we present the results of electron energy loss spectroscopy (EELS) analysis of composition and bonding s

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29

Bondar, Dmytro, Volodymyr Nadtoka, and Maksym Kraiev. "VACUUM SYSTEM FOR COATING PARTS OF ROCKET AND SPACE EQUIPMENT." Journal of Rocket-Space Technology 33, no. 4 (2024): 62–67. http://dx.doi.org/10.15421/452409.

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A vertical type vacuum plant was created for applying coatings using the ion-plasma deposition method to the inner surface of hollow products with a diameter of up to 200 mm and a length of up to 1000 mm. The plant includes: a vacuum chamber with a vacuum system, an evaporator with a magnetic system, a power supply and control system, a cooling system. Radial evaporation cathode of tubular shape with controlled arc is used. Inside the cathode is a magnetic system that controls the movement of cathode spots on its surface. Permanent magnets create arched magnetic fields that hold the position o

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30

Gortschakow, S., A. Khakpour, S. Popov, St Franke, R. Methling, and D. Uhrlandt. "Determination of Cr Density in the Active Phase of a High-current Vacuum Arcs." PLASMA PHYSICS AND TECHNOLOGY 4, no. 2 (2017): 190–93. http://dx.doi.org/10.14311/ppt.2017.2.190.

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Melting and evaporation of the anode surface strongly influence the interruption capability of vacuum circuit breakers, because they lead to injection of atomic vapour into the inter-electrode gap. Determination of the vapour density and its dynamics with respect to different anode phenomena is therefore of great importance. Results of Cr density measurements in a high-current vacuum arc by using broadband absorption spectroscopy are presented. The vapour density of atomic Cr is determined after the formation of anode spots as well as close to the current zero. Cr I resonance lines at 425.43 n

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31

Nagai, Hiroshi, Kazuhiko Majima, Masaru Yokota, et al. "Preparation of metallic magnetic fluid by vacuum evaporation and arc-plasma methods." Journal of the Japan Society of Powder and Powder Metallurgy 36, no. 6 (1989): 774–77. http://dx.doi.org/10.2497/jjspm.36.774.

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32

Xu, Ya, Jun You Yang, Masahiko Demura, Toru Hara, and Toshiyuki Hirano. "Synthesis of Ni-Al Intermetallic Nanoparticle Catalysts by Vacuum Arc Plasma Evaporation." Materials Science Forum 654-656 (June 2010): 2907–10. http://dx.doi.org/10.4028/www.scientific.net/msf.654-656.2907.

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In order to pursue high catalytic performance of Ni-Al intermetallic compounds for hydrogen production, we synthesized Ni-Al intermetallic nanoparticles from Ni-Al alloy ingots by vacuum arc plasma evaporation technique for the first time. The characterization of the synthesized nanoparticles was carried out using X-ray diffraction, scanning electron microscopy, transmission electron microscopy, energy dispersive X-ray spectroscopy. The catalytic properties of the Ni-Al nanoparticles for methanol decomposition were evaluated. It is found that the nanoparticles had a large surface area above 70

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33

Witke, T., and P. Siemroth. "Deposition of droplet-free films by vacuum arc evaporation-results and applications." IEEE Transactions on Plasma Science 27, no. 4 (1999): 1039–44. http://dx.doi.org/10.1109/27.782278.

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34

Vetter, J., T. Krug, and V. von der Heide. "AlTiCrNO coatings for dry cutting deposited by reactive cathodic vacuum arc evaporation." Surface and Coatings Technology 174-175 (September 2003): 615–19. http://dx.doi.org/10.1016/s0257-8972(03)00349-9.

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35

Čyvienė, J., M. Laurikaitis, and J. Dudonis. "Deposition of nanocomposite Zr–ZrO2 films by reactive cathodic vacuum arc evaporation." Materials Science and Engineering: B 118, no. 1-3 (2005): 238–41. http://dx.doi.org/10.1016/j.mseb.2004.12.036.

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36

Sue, J. Albert, Anthony J. Perry, and Jörg Vetter. "Young's modulus and stress of CrN deposited by cathodic vacuum arc evaporation." Surface and Coatings Technology 68-69 (December 1994): 126–30. http://dx.doi.org/10.1016/0257-8972(94)90149-x.

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37

Siefert, Wolfgang. "Anodic Arc Evaporation —A New Vacuum-Coating Technique for Textiles and Films." Journal of Coated Fabrics 23, no. 1 (1993): 30–33. http://dx.doi.org/10.1177/152808379302300105.

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38

Miyata, Toshihiro, Satoshi Ida, and Tadatsugu Minami. "High-rate deposition of ZnO thin films by vacuum arc plasma evaporation." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 21, no. 4 (2003): 1404–8. http://dx.doi.org/10.1116/1.1580492.

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39

Wang, Benfu, Xiubo Tian, Jian Hu, Chunzhi Gong, Xiangli Liu, and Jin Li. "Enhancement of discharge and mechanical properties of ta-C films by pulse-enhanced cathodic arc deposition." Journal of Vacuum Science & Technology A 41, no. 3 (2023): 033003. http://dx.doi.org/10.1116/6.0002352.

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A home-made straight-duct filter cathodic vacuum arc system was used to synthesize tetrahedral amorphous carbon (ta-C) films. The ta-C films were fabricated using both direct-current cathodic arc evaporation (DC-CAE) and pulse-enhanced cathodic arc evaporation. A series of films were prepared as a function of pulse current ranging from 500 to 1000 A compared with 80 A direct current. The introduction of pulse current could markedly increase instantaneous input power (Wiip). The pulse-enhanced Wiip led to the increase in average substrate current from 0.46 to 1.07 A. Moreover, compared with DC-

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40

Kostrin, D. K., and A. A. Lisenkov. "Synthesis of Transition Metals Carbide Compounds in the Vacuum Arc Discharge Plasma." Materials Science Forum 870 (September 2016): 371–76. http://dx.doi.org/10.4028/www.scientific.net/msf.870.371.

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To implement the plasmochemical synthesis of transition metals (Ti, Zr, Mo, W) carbide compounds in a plasma flux of the vacuum arc the discharge carbonaceous working gas is infused. It is shown that the composition of the initial carbonaceous gas defines both the carbon output, and the nature and course of the carbide compounds formation chemical reaction. The composition analysis of the plasma flux in the course of the coating evaporation was carried out by means of the developed emissive spectral analyzer. The result shows that a considerable part of transition metals carbide phases has wid

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41

Yamamoto, Shinji, Toru Iwao, and Yoshiyasu Ehara. "Evaporation Rate Affected by Current Density and Number of Vacuum Arc Cathode Spot." IEEJ Transactions on Power and Energy 136, no. 9 (2016): 755–60. http://dx.doi.org/10.1541/ieejpes.136.755.

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42

Ma, Yinghe, Jianguo Yang, Xiubo Tian, et al. "Influence of Acetylene on Ti Target Poisoning During Pulse-Enhanced Vacuum Arc Evaporation." IEEE Transactions on Plasma Science 48, no. 8 (2020): 2799–809. http://dx.doi.org/10.1109/tps.2020.3009155.

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43

Ma, Yinghe, Chunzhi Gong, Xiubo Tian, and Paul K. Chu. "Imaging and motion of cathode group spots during pulse-enhanced vacuum arc evaporation." Vacuum 139 (May 2017): 37–43. http://dx.doi.org/10.1016/j.vacuum.2017.02.008.

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44

Miyata, Toshihiro, Youhei Minamino, Satoshi Ida, and Tadatsugu Minami. "Highly transparent and conductive ZnO:Al thin films prepared by vacuum arc plasma evaporation." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 22, no. 4 (2004): 1711–15. http://dx.doi.org/10.1116/1.1759351.

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45

Miyata, Toshihiro, Yasunori Honma, and Tadatsugu Minami. "Preparation of transparent conducting B-doped ZnO films by vacuum arc plasma evaporation." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 25, no. 4 (2007): 1193–97. http://dx.doi.org/10.1116/1.2484424.

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46

Cao, Zhiyuan, Rui Li, Bo Cao, et al. "Hybrid plasma modeling of the interaction between the vacuum arc jet and the hot metallic particle near the current zero." Physics of Plasmas 29, no. 11 (2022): 113512. http://dx.doi.org/10.1063/5.0107444.

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In this paper, the interaction between the vacuum arc plasma jet and the hot metallic particle near current zero was investigated by numerical simulation. A vacuum arc plasma jet model was developed using the hybrid simulation method, in which electrons were considered as a massless fluid, while heavy particles such as atoms and ions were modeled as particles. In this model, the effect of the evaporation of metal atoms from the metallic particle was considered. Additionally, the Monte Carlo collision method was used to model inelastic collisions between electrons and heavy particles. The simul

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47

Suman, Choudhury, and Kumar Sinha Sanjay. "A COMPARATIVE STUDY OF MO FILMS DEPOSITED ON AISI 310 AND AL2O3 SURFACE USING ANODIC VACUUM ARC." International Journal of Multidisciplinary Research and Modern Education ( 4, no. 1 (2018): 146–51. https://doi.org/10.5281/zenodo.1288800.

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The Surface of Alumina and Stainless Steel was considered for thin film deposition of molybdenum by using Anodic Vacuum Arc. The evaporation was carried out at 0.07 mbar pressure and at a welding current of 60 Amperes where the temperature reached beyond 2500˚C and a thin layer of molybdenum was coated on the substrates. The corrosion rate, surface morphology, crystallite size and lattice strain were calculated by using Electrochemical Analyzer, Scanning Electron Microscope and X-Ray Diffraction respectively.

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48

Kang, Jang-Won, Jong Park, Byung Choe, et al. "Preparation of Spherical Mo5Si3 Powder by Inductively Coupled Thermal Plasma Treatment." Metals 8, no. 8 (2018): 604. http://dx.doi.org/10.3390/met8080604.

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A method was developed to fabricate spherical Mo5Si3 powder by milling and spheroidizing using inductively coupled thermal plasma. A Mo5Si3 alloy ingot was fabricated by vacuum arc melting, after which it was easily pulverized into powder by milling due to its brittle nature. The milled powders had an irregular shape, but after being spheroidized by the thermal plasma treatment, they had a spherical shape. Sphericity was increased with increasing plasma power. After plasma treatment, the percentage of the Mo3Si phase had increased due to Si evaporation. The possibility of Si evaporation was th

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49

Shin, Gi Won, Jae Hyeon Kim, Sun Hee Lee, et al. "Measurement of re-entry plasma density using microwave reflectometer in laboratory." Review of Scientific Instruments 93, no. 10 (2022): 103521. http://dx.doi.org/10.1063/5.0093263.

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A laboratory-scale experiment was conducted to reproduce plasma with properties similar to re-entry plasma and measure the plasma density using a microwave reflectometer system. To reproduce a similar re-entry plasma, a high-temperature refractory anode vacuum arc plasma method was used among arc plasma discharge methods, and arc plasma having high temperature, high speed, and high-density plasma characteristics was discharged inside a vacuum chamber. A hot refractory anode made of tungsten was used to show high-temperature plasma characteristics, and high-density plasma characteristics were d

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50

Tulina, A. A., A. Yu Nazarov, and V. R. Mukhamadeev. "Study of the properties of vacuum arc coatings based on the aluminum oxide system." Vestnik UGATU 27, no. 4(102) (2023): 144–51. http://dx.doi.org/10.54708/19926502_2023_274102144.

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The article describes the study of a coating based on aluminum oxide, obtained by the method of vacuum-arc evaporation on samples of hard alloy VK8 with different values of the bias voltage. A number of tests were carried out, including a scratch test, tribological tests in order to establish the nature of the wear of the coating with the coating technology used. The results showed that under the spraying and testing modes used, this coating is plastically deformed without showing the wear pattern standard for ceramic coatings

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