Shear localization in metallic materials at high strain rates

Na Yan, Zezhou Li, Yongbo Xu, Marc A. Meyers*

*Corresponding author for this work

Research output: Contribution to journalReview articlepeer-review

146 Citations (Scopus)

Abstract

Three factors govern adiabatic shear localization: strain hardening (or softening), strain-rate hardening, and thermal softening. It is typically associated with large shear strains (>1), high strain rates (103–107 s−1), and high temperatures (40–100% of melting point), all of which happen within narrow regions with widths of about 1–200 μm. It is often an undesirable phenomenon, leading to failure, but there are situations where it is desirable, e. g., the generation of machining chips. Here, we review the development of both theoretical and experimental achievements, from the initiation of shear bands to their propagation with emphasis on three aspects: novel experimental techniques, novel materials, and nano/microstructural effects. The principal characteristics of adiabatic shear bands in metallic materials at the nano- and micro-scale are described. Bands that were formerly identified as transformed actually consist of nanocrystalline/ultrafine grains. These grains result from the breakup of the microstructure by a rotational recrystallization process. The evolution of the microstructure inside shear bands and their interactions for hcp, bcc, and fcc alloys, high-entropy alloys, nanocrystalline alloys, and metallic glasses are analyzed mechanistically. The gaps in the field and opportunities for future research are identified. Modern experimental characterization and computational techniques enable a more profound and predictive understanding of adiabatic shear localization and its avoidance in advanced materials.

Original languageEnglish
Article number100755
JournalProgress in Materials Science
Volume119
DOIs
Publication statusPublished - Jun 2021
Externally publishedYes

Fingerprint

Dive into the research topics of 'Shear localization in metallic materials at high strain rates'. Together they form a unique fingerprint.

Cite this