Skip to main navigation Skip to search Skip to main content

Determination of dynamic flow stress equation based on discrete experimental data: Part 2 dynamic flow stress depending on strain, strain-rate and temperature

  • Xianglin Huang
  • , Q. M. Li*
  • *Corresponding author for this work
  • University of Manchester

Research output: Contribution to journal › Article › peer-review

Abstract

In this study, the effects of strain, strain-rate and temperature on the flow stress of C54400 phosphor copper alloy is investigated experimentally. Artificial neural network (ANN) is used to train the qualified data from the split Hopkinson pressure bar (SHPB) tests, obtaining finely-filled flow stress array (an order-three tensor). CANDECOM/PARAFAC (CP) decomposition method is used to decompose the flow stress array, from which both discrete and analytical expressions of flow stress equations are obtained. It is found that the analytical flow stress equation (f(ε,ε˙,T)Ana_R2) based on CP Rank-2 decomposition agrees well with the finely-filled data from ANN. Most importantly, the thermal softening effect of the C54400 material is well reproduced by f(ε,ε˙,T)Ana_R2. Finally, f(ε,ε˙,T)Ana_R2 is compared with the flow stress equation (f(ε,ε˙,T)MJC) obtained by following the conventional method to determine the dynamic flow stress. Results show the excellent performance of f(ε,ε˙,T)Ana_R2 in flow stress prediction from low to high temperatures while f(ε,ε˙,T)MJC fails in the high temperature range. The comparison demonstrates the effectiveness of the proposed framework in the determination of dynamic flow stress equations.

Original languageEnglish
Article number105432
JournalInternational Journal of Impact Engineering
Volume206
DOIs
Publication statusPublished - Dec 2025
Externally publishedYes

Keywords

  • Artificial neural network (ANN)
  • CANDECOM/PARAFAC (CP)
  • Dynamic flow stress
  • Split Hopkinson pressure bar (SHPB)
  • Strain-rate effect
  • Thermal effect

Fingerprint

Dive into the research topics of 'Determination of dynamic flow stress equation based on discrete experimental data: Part 2 dynamic flow stress depending on strain, strain-rate and temperature'. Together they form a unique fingerprint.

Cite this