4.7 Article

Microstructure evolution during austenite reversion in Fe-Ni martensitic alloys

Journal

ACTA MATERIALIA
Volume 144, Issue -, Pages 269-280

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.actamat.2017.10.068

Keywords

Reverse transformation; Austenite memory; Recrystallization; In-situ observation; Crystallography

Funding

  1. Japan Society for the Promotion of Science (JSPS)
  2. Ministry of Education, Culture Sports, Science and Technology [23360316, 25630315]
  3. Grants-in-Aid for Scientific Research [17K14842, 23360316, 25630315] Funding Source: KAKEN

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The change of microstructure during reverse transformation by continuous heating and isothermal holding above A(f) temperature were studied in Fe-11,18 and 23 Ni (mass %) alloys. In-situ observation by using confocal laser scanning microscopy (CLSM) and in-situ/ex-situ electron backscatter diffraction (EBSD) analysis were used for direct observation of reverse transformation. It was found that the start temperatures (As) for austenite reversion decrease with increasing of Ni content while they are higher than To temperatures. Reverse transformation in the Fe-23 Ni alloy is accompanied with a sharp surface relief indicating that reverse transformation occurs martensitically in this alloy. EBSD measurements show that reversed austenite grains in this alloy are formed with nearly identical crystallographic orientations to the prior one, which means orientations and boundaries of prior austenite grains are preserved due to the austenite memory effect. By further holding above Af temperature spontaneous recrystallization of reverted austenite proceeds. The Fe-18 Ni alloy also shows similar microstructure change during reversion. Near Kurdjamov-Sachs (K-S) orientation relationship is found between reversed austenite and initial martensite during reversion of the Fe-18 and 23 Ni alloys. However, when the Ni content is decreased to 11%, no specific orientation relationship is found between reversed austenite and initial martensite, indicating that the reversion mechanism is changed from martensitic to partitionless diffusional (massive) mechanism. (C) 2017 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.

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