2019
DOI: 10.3103/s1068375519050077
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Mathematical Modeling of Roughness Changing of Hard Metal Coatings Obtained by Contactless Electrospark Deposition

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Cited by 2 publications
(8 citation statements)
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“…With an increase in the pulse energy, an increase in the diameter and time of the spark discharge occurs, as a result of which the erosion of the electrodes increases. The depth and size of the craters of the solidified material on the cathode grows and, as a result, the roughness increases [6][7][8][9][14][15]. In the ESD of the samples with initial roughness Ra=1.67, 2.5 and 3 μm, the roughness Ra of the coatings of all used electrodes at pulse energy up to 0.03 J is close to that of the initial titanium surface (Fig.…”
Section: J)mentioning
confidence: 92%
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“…With an increase in the pulse energy, an increase in the diameter and time of the spark discharge occurs, as a result of which the erosion of the electrodes increases. The depth and size of the craters of the solidified material on the cathode grows and, as a result, the roughness increases [6][7][8][9][14][15]. In the ESD of the samples with initial roughness Ra=1.67, 2.5 and 3 μm, the roughness Ra of the coatings of all used electrodes at pulse energy up to 0.03 J is close to that of the initial titanium surface (Fig.…”
Section: J)mentioning
confidence: 92%
“…It is known [6][7][8][9][15][16][17][18][19][20][21][22][23][24][25] that the increase in energy leads to an increase in the thickness, hardness and amount of wear-resistant phases in the coatings, which creates prerequisites for increased wear resistance of the coated surfaces. At the same time, however, the roughness and unevenness of the coatings increases.…”
Section: J)mentioning
confidence: 99%
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