<p>In this paper, the formation mechanism of <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(1/6&lt;11\overline{2 }]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>6</mn> <mo>&lt;</mo> <mn>11</mn> <mover> <mn>2</mn> <mo>¯</mo> </mover> <mrow> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> Shockley partial dislocation bow-outs in the γ phase of TiAl alloys was investigated during the warm shot peening (WSP). The movement of such partial dislocations was attributed to the formation of dislocation bow-outs, specifically triangular and trapezoidal ones. Each bow-out consisted of stacking faults (complete and incomplete) and a dislocation configuration (triangular or trapezoidal). Therefore, the formation energy of the bow-outs was obtained by calculating the energy summation of these stacking faults and dislocation configurations. By deducing and analyzing the formation energy, a critical bow-out angle was proposed to characterize the stability of the dislocation bowing. During the Shockley partial dislocation bowing process, the lattice changes in front of the stacking fault were revealed. The complex trajectories of Ti and Al atoms during these lattice changes were attributed to the coupling of lattice distortion and shear under the impact of shots.</p> Graphical abstract <p></p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Study on dislocation bow-out induced Shockley partial dislocation movement of γ phase in TiAl alloys

  • Yang Qiao,
  • Daosheng Wen,
  • Beibei Kong,
  • Qinghua Lv,
  • Yuhang Wang,
  • Zhen Gong,
  • Yanxing Ding,
  • Minghao Zhang

摘要

In this paper, the formation mechanism of \(1/6<11\overline{2 }]\) 1 / 6 < 11 2 ¯ ] Shockley partial dislocation bow-outs in the γ phase of TiAl alloys was investigated during the warm shot peening (WSP). The movement of such partial dislocations was attributed to the formation of dislocation bow-outs, specifically triangular and trapezoidal ones. Each bow-out consisted of stacking faults (complete and incomplete) and a dislocation configuration (triangular or trapezoidal). Therefore, the formation energy of the bow-outs was obtained by calculating the energy summation of these stacking faults and dislocation configurations. By deducing and analyzing the formation energy, a critical bow-out angle was proposed to characterize the stability of the dislocation bowing. During the Shockley partial dislocation bowing process, the lattice changes in front of the stacking fault were revealed. The complex trajectories of Ti and Al atoms during these lattice changes were attributed to the coupling of lattice distortion and shear under the impact of shots.

Graphical abstract