Lath formation mechanisms and twinning as lath martensite substructures in an ultra low-carbon iron alloy

Lath martensite is the dominant microstructural feature in quenched low-carbon Fe-C alloys. Its formation mechanism is not clear, despite extensive research. The microstructure of an Fe-0.05 C (wt.%) alloy water-quenched at various austenitizing temperatures has been investigated using transmission...

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Veröffentlicht in:Scientific reports 2018-09, Vol.8 (1), p.14264-11, Article 14264
Hauptverfasser: Ping, D. H., Guo, S. Q., Imura, M., Liu, X., Ohmura, T., Ohnuma, M., Lu, X., Abe, T., Onodera, H.
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container_title Scientific reports
container_volume 8
creator Ping, D. H.
Guo, S. Q.
Imura, M.
Liu, X.
Ohmura, T.
Ohnuma, M.
Lu, X.
Abe, T.
Onodera, H.
description Lath martensite is the dominant microstructural feature in quenched low-carbon Fe-C alloys. Its formation mechanism is not clear, despite extensive research. The microstructure of an Fe-0.05 C (wt.%) alloy water-quenched at various austenitizing temperatures has been investigated using transmission electron microscopy and a novel lath formation mechanism has been proposed. Body-centered cubic {112}〈111〉-type twin can be retained inside laths in the samples quenched at temperatures from 1050 °C to 1200 °C. The formation mechanism of laths with a twin substructure has been explained based on the twin structure as an initial product of martensitic transformation. A detailed detwinning mechanism in the auto-tempering process has also been discussed, because auto-tempering is inevitable during the quenching of low-carbon Fe-C alloys. The driving force for the detwinning is the instability of ω-Fe(C) particles, which are located only at the twinning boundary region. The twin boundary can move through the ω ↔ bcc transition in which the ω phase region represents the twin boundary.
doi_str_mv 10.1038/s41598-018-32679-6
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A detailed detwinning mechanism in the auto-tempering process has also been discussed, because auto-tempering is inevitable during the quenching of low-carbon Fe-C alloys. The driving force for the detwinning is the instability of ω-Fe(C) particles, which are located only at the twinning boundary region. 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H.</au><au>Guo, S. Q.</au><au>Imura, M.</au><au>Liu, X.</au><au>Ohmura, T.</au><au>Ohnuma, M.</au><au>Lu, X.</au><au>Abe, T.</au><au>Onodera, H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Lath formation mechanisms and twinning as lath martensite substructures in an ultra low-carbon iron alloy</atitle><jtitle>Scientific reports</jtitle><stitle>Sci Rep</stitle><addtitle>Sci Rep</addtitle><date>2018-09-24</date><risdate>2018</risdate><volume>8</volume><issue>1</issue><spage>14264</spage><epage>11</epage><pages>14264-11</pages><artnum>14264</artnum><issn>2045-2322</issn><eissn>2045-2322</eissn><abstract>Lath martensite is the dominant microstructural feature in quenched low-carbon Fe-C alloys. Its formation mechanism is not clear, despite extensive research. 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The twin boundary can move through the ω ↔ bcc transition in which the ω phase region represents the twin boundary.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>30250050</pmid><doi>10.1038/s41598-018-32679-6</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-2608-1473</orcidid><orcidid>https://orcid.org/0000-0002-2933-1976</orcidid><oa>free_for_read</oa></addata></record>
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subjects 639/301/1023/1026
639/301/357/537
Alloys
Carbon
Humanities and Social Sciences
Microstructure
multidisciplinary
Science
Science (multidisciplinary)
Transmission electron microscopy
title Lath formation mechanisms and twinning as lath martensite substructures in an ultra low-carbon iron alloy
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