Structure of the Contact Layers of Steel and Their Deterioration in Dry Sliding Against Steel Under High-Density Electric Currents at Different Turn Ratios of a Supply Transformer
The structural states of the contact layers of C235 steel in dry sliding against C45 steel are studied under a high-density alternating electric current. A sliding electrical contact is made in the secondary winding circuit of a power transformer. The electrical conductivity of this contact decrease...
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Veröffentlicht in: | Russian physics journal 2024, Vol.67 (1), p.1-8 |
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description | The structural states of the contact layers of C235 steel in dry sliding against C45 steel are studied under a high-density alternating electric current. A sliding electrical contact is made in the secondary winding circuit of a power transformer. The electrical conductivity of this contact decreases with a decrease in the turn ratio. At the same time, the wear resistance and the current density corresponding to the onset of catastrophic wear also decrease. The formation of FeO on the contact surface is shown. The FeO content is observed to increase with the decreasing turn ratio. This is one of the reasons for the decrease in the contact electrical conductivity. Another reason is an increase in the displacement current and a corresponding increase in the excitation of the FeO atomic lattice with a decrease in the turn ratio. The peculiarities of the sliding surface morphology are presented in order to identify the mechanism of the contact layer deterioration and find other reasons for the decrease in the contact electrical conductivity with the decreasing turn ratio. However, the surface layer morphology does not change with the changing turn ratio in sliding under a current density higher than 100 A/cm
2
. Two sectors appear on the nominal contact area. The boundary between the sectors is quite distinct and is perpendicular to the sliding direction. The sector directed towards the running up contact surface of the counterbody has traces of adhesion, plowing, etc., which generally appear during plastic deformation of the contact surface. The other sector shows the signs of deformation similar to that of a viscous liquid. No traces of adhesion are observed. |
doi_str_mv | 10.1007/s11182-024-03081-9 |
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2
. Two sectors appear on the nominal contact area. The boundary between the sectors is quite distinct and is perpendicular to the sliding direction. The sector directed towards the running up contact surface of the counterbody has traces of adhesion, plowing, etc., which generally appear during plastic deformation of the contact surface. The other sector shows the signs of deformation similar to that of a viscous liquid. No traces of adhesion are observed.</description><identifier>ISSN: 1064-8887</identifier><identifier>EISSN: 1573-9228</identifier><identifier>DOI: 10.1007/s11182-024-03081-9</identifier><language>eng</language><publisher>Cham: Springer International Publishing</publisher><subject>Adhesion ; Catastrophic wear ; Circuits ; Condensed Matter Physics ; Condensed-State Physics ; Current density ; Electric contacts ; Electric currents ; Electrical resistivity ; Hadrons ; Heavy Ions ; High density ; Lasers ; Mathematical and Computational Physics ; Medium carbon steels ; Morphology ; Nuclear Physics ; Optical Devices ; Optics ; Photonics ; Physics ; Physics and Astronomy ; Plastic deformation ; Plowing ; Sliding ; Surface layers ; Theoretical ; Transformers ; Wear resistance</subject><ispartof>Russian physics journal, 2024, Vol.67 (1), p.1-8</ispartof><rights>The Author(s), under exclusive licence to Springer Nature Switzlerland AG 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c270t-f3cf36b5d2a9a30af18f167aeb92a7c371623c503a63546373ca9c165a1acc653</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11182-024-03081-9$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11182-024-03081-9$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Aleutdinova, M. I.</creatorcontrib><creatorcontrib>Fadin, V. V.</creatorcontrib><title>Structure of the Contact Layers of Steel and Their Deterioration in Dry Sliding Against Steel Under High-Density Electric Currents at Different Turn Ratios of a Supply Transformer</title><title>Russian physics journal</title><addtitle>Russ Phys J</addtitle><description>The structural states of the contact layers of C235 steel in dry sliding against C45 steel are studied under a high-density alternating electric current. A sliding electrical contact is made in the secondary winding circuit of a power transformer. The electrical conductivity of this contact decreases with a decrease in the turn ratio. At the same time, the wear resistance and the current density corresponding to the onset of catastrophic wear also decrease. The formation of FeO on the contact surface is shown. The FeO content is observed to increase with the decreasing turn ratio. This is one of the reasons for the decrease in the contact electrical conductivity. Another reason is an increase in the displacement current and a corresponding increase in the excitation of the FeO atomic lattice with a decrease in the turn ratio. The peculiarities of the sliding surface morphology are presented in order to identify the mechanism of the contact layer deterioration and find other reasons for the decrease in the contact electrical conductivity with the decreasing turn ratio. However, the surface layer morphology does not change with the changing turn ratio in sliding under a current density higher than 100 A/cm
2
. Two sectors appear on the nominal contact area. The boundary between the sectors is quite distinct and is perpendicular to the sliding direction. The sector directed towards the running up contact surface of the counterbody has traces of adhesion, plowing, etc., which generally appear during plastic deformation of the contact surface. The other sector shows the signs of deformation similar to that of a viscous liquid. No traces of adhesion are observed.</description><subject>Adhesion</subject><subject>Catastrophic wear</subject><subject>Circuits</subject><subject>Condensed Matter Physics</subject><subject>Condensed-State Physics</subject><subject>Current density</subject><subject>Electric contacts</subject><subject>Electric currents</subject><subject>Electrical resistivity</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>High density</subject><subject>Lasers</subject><subject>Mathematical and Computational Physics</subject><subject>Medium carbon steels</subject><subject>Morphology</subject><subject>Nuclear Physics</subject><subject>Optical Devices</subject><subject>Optics</subject><subject>Photonics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Plastic deformation</subject><subject>Plowing</subject><subject>Sliding</subject><subject>Surface layers</subject><subject>Theoretical</subject><subject>Transformers</subject><subject>Wear resistance</subject><issn>1064-8887</issn><issn>1573-9228</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp9kU1v00AQhi0EEqXwBziNxHlhP-y1fayS0iJFQiLpeTXdzCZbueswuz74d_EHcZpK3DjNh97nnZHeqvqs5FclZfstK6U6LaSuhTSyU6J_U12ppjWi17p7u_TS1qLruvZ99SHnJykXzLZX1Z9t4cmXiQnGAOVIsBpTQV9ggzNxPm-3hWgATHvYHSkyrKkQx5GxxDFBTLDmGbZD3Md0gJsDxpTLK_SQ9sRwHw9HsaaUY5nhdiBfOHpYTcyUSgYssI4h0HmC3cQJfp2tX24jbKfTaZhhx5hyGPmZ-GP1LuCQ6dNrva4evt_uVvdi8_Pux-pmI7xuZRHB-GDsY7PX2KORGFQXlG2RHnuNrTetstr4Rhq0pqmtaY3H3ivboELvbWOuqy8X3xOPvyfKxT2Ny3fLSad73TR1baxdVPqi8jzmzBTcieMz8uyUdOdw3CUct4TjXsJx_QKZC5QXcToQ_7P-D_UX0m-Ucg</recordid><startdate>2024</startdate><enddate>2024</enddate><creator>Aleutdinova, M. I.</creator><creator>Fadin, V. V.</creator><general>Springer International Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>2024</creationdate><title>Structure of the Contact Layers of Steel and Their Deterioration in Dry Sliding Against Steel Under High-Density Electric Currents at Different Turn Ratios of a Supply Transformer</title><author>Aleutdinova, M. I. ; Fadin, V. V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c270t-f3cf36b5d2a9a30af18f167aeb92a7c371623c503a63546373ca9c165a1acc653</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Adhesion</topic><topic>Catastrophic wear</topic><topic>Circuits</topic><topic>Condensed Matter Physics</topic><topic>Condensed-State Physics</topic><topic>Current density</topic><topic>Electric contacts</topic><topic>Electric currents</topic><topic>Electrical resistivity</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>High density</topic><topic>Lasers</topic><topic>Mathematical and Computational Physics</topic><topic>Medium carbon steels</topic><topic>Morphology</topic><topic>Nuclear Physics</topic><topic>Optical Devices</topic><topic>Optics</topic><topic>Photonics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Plastic deformation</topic><topic>Plowing</topic><topic>Sliding</topic><topic>Surface layers</topic><topic>Theoretical</topic><topic>Transformers</topic><topic>Wear resistance</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Aleutdinova, M. I.</creatorcontrib><creatorcontrib>Fadin, V. V.</creatorcontrib><collection>CrossRef</collection><jtitle>Russian physics journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Aleutdinova, M. I.</au><au>Fadin, V. V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structure of the Contact Layers of Steel and Their Deterioration in Dry Sliding Against Steel Under High-Density Electric Currents at Different Turn Ratios of a Supply Transformer</atitle><jtitle>Russian physics journal</jtitle><stitle>Russ Phys J</stitle><date>2024</date><risdate>2024</risdate><volume>67</volume><issue>1</issue><spage>1</spage><epage>8</epage><pages>1-8</pages><issn>1064-8887</issn><eissn>1573-9228</eissn><abstract>The structural states of the contact layers of C235 steel in dry sliding against C45 steel are studied under a high-density alternating electric current. A sliding electrical contact is made in the secondary winding circuit of a power transformer. The electrical conductivity of this contact decreases with a decrease in the turn ratio. At the same time, the wear resistance and the current density corresponding to the onset of catastrophic wear also decrease. The formation of FeO on the contact surface is shown. The FeO content is observed to increase with the decreasing turn ratio. This is one of the reasons for the decrease in the contact electrical conductivity. Another reason is an increase in the displacement current and a corresponding increase in the excitation of the FeO atomic lattice with a decrease in the turn ratio. The peculiarities of the sliding surface morphology are presented in order to identify the mechanism of the contact layer deterioration and find other reasons for the decrease in the contact electrical conductivity with the decreasing turn ratio. However, the surface layer morphology does not change with the changing turn ratio in sliding under a current density higher than 100 A/cm
2
. Two sectors appear on the nominal contact area. The boundary between the sectors is quite distinct and is perpendicular to the sliding direction. The sector directed towards the running up contact surface of the counterbody has traces of adhesion, plowing, etc., which generally appear during plastic deformation of the contact surface. The other sector shows the signs of deformation similar to that of a viscous liquid. No traces of adhesion are observed.</abstract><cop>Cham</cop><pub>Springer International Publishing</pub><doi>10.1007/s11182-024-03081-9</doi><tpages>8</tpages></addata></record> |
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subjects | Adhesion Catastrophic wear Circuits Condensed Matter Physics Condensed-State Physics Current density Electric contacts Electric currents Electrical resistivity Hadrons Heavy Ions High density Lasers Mathematical and Computational Physics Medium carbon steels Morphology Nuclear Physics Optical Devices Optics Photonics Physics Physics and Astronomy Plastic deformation Plowing Sliding Surface layers Theoretical Transformers Wear resistance |
title | Structure of the Contact Layers of Steel and Their Deterioration in Dry Sliding Against Steel Under High-Density Electric Currents at Different Turn Ratios of a Supply Transformer |
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