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Nano-creep behavior of Ti-based bulk amorphous alloy after electrochemical hydrogen charging

  • Fuyu Dong
  • , Guishen Zhou
  • , Yuanhong Hu
  • , Yue Zhang*
  • , Kun Liu
  • , Binbin Wang
  • , Liangshun Luo
  • , Yanqing Su
  • , Xiaoguang Yuan
  • , Peng Kuang
  • , Peng Zhang
  • , Xingzhong Cao*
  • , Jun Cheng
  • *Corresponding author for this work
  • Shenyang University of Technology
  • Harbin Institute of Technology
  • CAS - Institute of High Energy Physics
  • Northwest Institute for Nonferrous Metal Research

Research output: Contribution to journalArticlepeer-review

Abstract

In the present study, a Ti32.85Zr30.21Cu9Ni5.28Be22.66 bulk amorphous alloy was hydrogenated by the electrochemical method. Samples with different H content were obtained by changing the H-charging current density and charging time. X-ray diffraction (XRD), nanoindentation, and positron annihilation experiments were used to investigate the amorphous structure, nanomechanical properties, and positron annihilation behavior of the Ti32.85Zr30.21Cu9Ni5.28Be22.66 bulk amorphous alloy after electrochemical hydrogenation treatment. XRD analysis showed that the sample has an amorphous structure after hydrogen charging. Investigation of the nano-creep behavior using a nanoindentation instrument demonstrated that the creep displacement of the amorphous alloy decreases gradually with the increase of hydrogen content, and the creep stress index increases first and then decreases. The addition of hydrogen atoms inhibits the formation of the shear transformation zone (STZ), resulting in a decrease in the size and dimensions of STZ in the amorphous alloy and an increase in the activation energy. Three lifetime components were observed in the uncharged and charged samples, indicating the presence of three size ranges of open volume sites. The average annihilation lifetime of positrons decreases with the increase of current density and time of electrochemical hydrogen charging, indicating that the addition of hydrogen weakens the annihilation behavior of positrons. The defect range of the corresponding amorphous alloy decreases, making the creep behavior difficult to carry out. Compared with the uncharged hydrogenated sample, the Doppler broadening spectra showed that the hydrogenated sample contributes more to the positron annihilation of the core electrons, that is, the W parameter becomes larger and the S parameter becomes smaller. Although the addition of hydrogen affects the positron annihilation behavior, no new defects are generated in the amorphous alloy.

Original languageEnglish
Pages (from-to)529-537
Number of pages9
JournalInternational Journal of Hydrogen Energy
Volume101
DOIs
StatePublished - 3 Feb 2025
Externally publishedYes

UN SDGs

This output contributes to the following UN Sustainable Development Goals (SDGs)

  1. SDG 7 - Affordable and Clean Energy
    SDG 7 Affordable and Clean Energy

Keywords

  • Creep
  • Electrochemical hydrogen charging
  • Nanoindentation
  • Positron annihilation
  • Ti-based amorphous alloy

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