Abstract

The martensite-to-austenite reversion mechanisms under continuous heating and annealing of metastable austenitic stainless steel subjected to cold swaging were studied. The reversion-temperature-time diagram was constructed using high-resolution dilatometry. The diagram revealed a sequence of martensitic and diffusional reversion and recrystallization. Martensitic and diffusional reversion might be separated by using the heating rate of >10 °C/s. The reversion started via the martensitic mechanism, and the diffusional mechanism developed during subsequent heating. However, both mechanisms enhance simultaneously during continuous heating at slow heating rates (<10 °C/s). At higher temperatures, recrystallization occurred. Post-mortem microstructure analysis has allowed classifying the reverse annealing modes into low- (500–650 °C), medium- (~700 °C), and high-temperature (~800 °C) regimes. During low-temperature annealing, the development of the phase reversion, recovery, recrystallization, and carbide precipitation was characterized by both a high amount of new austenite grains and restriction of their growth that resulted in the formation of an ultrafine grain structure with an average grain size of 100–200 nm. Medium-temperature annealing was associated with the formation of almost a fully recrystallized austenitic structure, but the lamellar regions were still detected. Austenitic grain growth and dissolution of carbide particles were enhanced during high-temperature annealing.

Highlights

  • Metastable austenitic stainless (MAS) steels have a very attractive combination of properties such as high ductility and impact toughness, excellent corrosion and oxidation resistance, good weldability, and superior formability [1,2]

  • The start of the first reversion stage (St1) did not depend on the heating rate, but the finish of it increased with the rising of the heating rate as well as the start and finish of the second reversion stage (St2) and the temperature range of recrystallization (RX)

  • The heating with a rate higher than ~10 ◦C/s was associated with the development of both reversion mechanisms separately

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Summary

Introduction

Metastable austenitic stainless (MAS) steels have a very attractive combination of properties such as high ductility and impact toughness, excellent corrosion and oxidation resistance, good weldability, and superior formability [1,2]. They exhibit low yield strength that inhibits their application as a structural material. Substructure, and deformation band formation, deformationinduced γ→α’ transformation occurs during SPD [11,12,13,14]. It was reported [13,14] that austenite with face-centered cubic (FCC) lattice and deformation-induced martensite (DIM) with body-centered tetragonal (BCT) lattice are related through the Kurdjumov-Sachs (K-S)

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