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Slip- and Twinning-Related Dissipation in AZ31B Magnesium Alloy

Michał Maj, Sandra Musiał, Marcin Nowak

Abstract

Energy conversion in AZ31B magnesium alloy depends strongly on the dominant deformation mechanism. In slip-dominated specimen, strained parallel to extrusion direction $\parallel$ ED, approximately 50$\%$ of plastic work is converted into heat, with Taylor-Quinney coefficient $β_{int}$ rising rapidly then gradually with strain. Twinning-dominated specimen ($\perp$ ED) initially stores most plastic work, showing minimal heat dissipation, reflecting the dislocation-mediated nature of twinning in HCP metals, and $β_{int}$ increasing to $\approx$ 0.4 at failure. The final microstructure tracks stored energy evolution: the $\parallel$ ED specimen, predominantly slip-dominated, exhibits fragmented grains and strong dislocation activity, with twinning appearing at the final stages, driving energy accumulation and lattice rotation. In contrast, the $\perp$ ED specimen shows limited refinement, early localization, and twinning-driven premature fracture.

Slip- and Twinning-Related Dissipation in AZ31B Magnesium Alloy

Abstract

Energy conversion in AZ31B magnesium alloy depends strongly on the dominant deformation mechanism. In slip-dominated specimen, strained parallel to extrusion direction ED, approximately 50 of plastic work is converted into heat, with Taylor-Quinney coefficient rising rapidly then gradually with strain. Twinning-dominated specimen ( ED) initially stores most plastic work, showing minimal heat dissipation, reflecting the dislocation-mediated nature of twinning in HCP metals, and increasing to 0.4 at failure. The final microstructure tracks stored energy evolution: the ED specimen, predominantly slip-dominated, exhibits fragmented grains and strong dislocation activity, with twinning appearing at the final stages, driving energy accumulation and lattice rotation. In contrast, the ED specimen shows limited refinement, early localization, and twinning-driven premature fracture.
Paper Structure (1 section, 2 equations, 4 figures, 1 table)

This paper contains 1 section, 2 equations, 4 figures, 1 table.

Table of Contents

  1. Acknowledgements

Figures (4)

  • Figure 1: Specimen placement and initial microstructure (a) along with the experimental setup for heat sources determination and specimen dimensions (b).
  • Figure 2: Stress-strain curves for slip-dominated ($\parallel$ ED) and twinning-dominated ($\perp$ ED) loading directions, with the corresponding strain hardening coefficients ${d\sigma}$/${d\varepsilon}$ and mean temperature changes $\Delta T_{mean}$ (a). Corresponding fracture surfaces (b) and the distributions of the axial component of Hencky strain rate $\dot{\varepsilon}_{yy}$, and temperature gradient $\nabla_{y} T$ (c).
  • Figure 3: Plastic work $w_p$, energy dissipated as heat $q_d$ and stored energy $e_s$ as functions of plastic strain for slip-dominated ($\parallel$ ED) (a) and twinning-dominated ($\perp$ ED) specimens (b), along with the corresponding evolution of the integral $\beta_{int}$ and differential $\beta_{diff}$ Taylor-Quinney coefficients (c).
  • Figure 4: Microstructure after deformation shown as inverse pole figures projected along the straining direction along with pole figures evolution, for specimens strained ($\parallel$ ED) (a) and ($\perp$ ED) (b).