Skip to content
DraconiticResearch
Search Sources API
182,544 studies31 sourcesUpdated 58 min ago
PreprintCC BY 4.0arXiv

The Case Against Hall-Petch Hardening in High Entropy Carbide Ceramics

Abstract

Grain size is often used with the Hall-Petch relationship to justify differences in hardness in ceramic materials. Herein, hardness does not vary systematically with grain-size for fully dense, single-phase (Cr,Mo,Ta,V,W)C1-δ high entropy carbide ceramics for grain sizes that varied by a factor of three. Fully dense, single-phase ceramics with grain sizes from 9.3+/-0.3 to 28.8+/-0.7 microns exhibited a pronounced indentation size effect, with Vickers hardness decreasing from ~28-30 GPa at 0.49 N to ~20-21 GPa at 9.81 N, and Berkovich nanohardness ranging from 26 to 30 GPa at 10 mN. However, at a given load, hardness remained within a narrow range across the grain-size series, and no consistent Hall-Petch dependence was resolved. The lack of grain-size dependence likely indicates that the deformation volume sampled by the indenter was not controlled by grain-boundary interactions; instead, hardness was governed primarily by indentation load and local response of the rock salt carbide matrix.

Related

  1. Grain-Size Dependence of Thermal and Electrical Properties in (Cr,Mo,Ta,V,W)C1-δ High-Entropy Carbide Ceramics
    Ali Sarikhani, Gregory E. Hilmas, David W. Lipke +4
    arXivPreprintCC BY 4.0Full textCondensed matterarXiv
  2. Quantum spectral thermodynamics and active learning enable million-scale exploration of high-entropy ceramics
    Jie Sun, Yiheng Shen
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
  3. Multi-Fidelity Machine Learning for Predicting Startup Stress Growth and Strain Hardening in Wormlike Micellar Solutions
    Saghar Zolfaghari, Nunzia Lauriello, Ilaria Cusano +3
    arXivPreprintCC BY-NC-ND 4.0Full textCondensed matterarXiv
  4. Joint-decoupled iterative CBCT reconstruction with hybrid scatter estimation and voxel-adaptive beam hardening correction
    Jianing Sun, Jean Michel Létang, Qixiang Sun +3
    arXivPreprintarXiv licenceFull textBiological & medical physicsarXiv
  5. Scalable integration of silicon carbide color centers into nanophotonic structures
    Raphael Wörnle, Jonas Schmid, Dennis Grüner +7
    arXivPreprintCC BY 4.0Full textQuantum physics & quantum informationarXiv
BibTeX
@misc{sarikhani2026case,
  title = {{The Case Against Hall-Petch Hardening in High Entropy Carbide Ceramics}},
  author = {Ali Sarikhani and Ana C. Feltrin and Gregory E. Hilmas and David W. Lipke and Douglas E. Wolfe and Stefano Curtarolo and Shen J. Dillon and William G. Fahrenholtz},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.15717},
  eprint = {2609.15717},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.15717},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - The Case Against Hall-Petch Hardening in High Entropy Carbide Ceramics
AU  - Ali Sarikhani
AU  - Ana C. Feltrin
AU  - Gregory E. Hilmas
AU  - David W. Lipke
AU  - Douglas E. Wolfe
AU  - Stefano Curtarolo
AU  - Shen J. Dillon
AU  - William G. Fahrenholtz
PY  - 2026
DA  - 2026/09/14
PB  - arXiv
DO  - 10.48550/arxiv.2609.15717
UR  - https://arxiv.org/abs/2609.15717
AB  - Grain size is often used with the Hall-Petch relationship to justify differences in hardness in ceramic materials. Herein, hardness does not vary systematically with grain-size for fully dense, single-phase (Cr,Mo,Ta,V,W)C1-δ high entropy carbide ceramics for grain sizes that varied by a factor of three. Fully dense, single-phase ceramics with grain sizes from 9.3+/-0.3 to 28.8+/-0.7 microns exhibited a pronounced indentation size effect, with Vickers hardness decreasing from ~28-30 GPa at 0.49 N to ~20-21 GPa at 9.81 N, and Berkovich nanohardness ranging from 26 to 30 GPa at 10 mN. However, at a given load, hardness remained within a narrow range across the grain-size series, and no consistent Hall-Petch dependence was resolved. The lack of grain-size dependence likely indicates that the deformation volume sampled by the indenter was not controlled by grain-boundary interactions; instead, hardness was governed primarily by indentation load and local response of the rock salt carbide matrix.
ER  -