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Achieving cryogenic wear resistance of MoS2 beyond conventional lubricity: An atomistic simulation study

  • Zikun Tang
  • , Longhui Zhu
  • , Dongpeng Hua
  • , Zhenyuan Liang
  • , Jincheng Li
  • , Junpeng Gao
  • , Liqiang Chai
  • , Peng Wang
  • , Quan Xu
  • , Qing Zhou
  • , Sergey Lezhnev
  • , Evgeny Trofimov
  • Northwestern Polytechnical University Xian
  • City University of Hong Kong
  • CAS - Lanzhou Institute of Chemical Physics
  • China Aerospace Science and Technology Corporation
  • Rudny Industrial Institute
  • South Ural State University

Research output: Contribution to journalArticlepeer-review

1 Scopus citations

Abstract

Molybdenum disulfide MoS2 is an attractive solid lubricant because weak interlayer interactions enable easy shear, yet its wear resistance deteriorates at low temperatures. Ti doping serves as a microstructural design strategy to strengthen MoS2 for cryogenic service. Experiments and simulations show that dispersed Ti modifies local bonding, induces Ti-S coordinated configurations, and builds an interlayer network of Ti, S, and Ti-S clusters. This nanoscale architecture raises hardness to 1.93 GPa and elastic modulus to 45.30 GPa through lattice distortion and strong pinning that hinder interlayer shear. Although the strengthened interface increases the friction coefficient, it markedly lowers wear at 223 K. Atomistic simulations reveal a transition from progressive interlayer sliding and local delamination in pristine MoS2 to coherent block-like deformation of pinned layers, which promotes more uniform stress accommodation. The associated increase in bending stiffness also suppresses wrinkling, offering a clear design route for durable solid-lubricant coatings in low-temperature environments.

Original languageEnglish
Article number112053
JournalTribology International
Volume221
DOIs
StatePublished - Sep 2026

Keywords

  • Cryogenic tribological performance
  • Molecular dynamics simulations
  • Molybdenum disulfide coating
  • Solid lubricant coating
  • Tribology

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