1 / 20

Atomistic Mechanisms for Grain Boundary Migration

Atomistic Mechanisms for Grain Boundary Migration  Overview of Atomistic Simulations of Grain Boundary Migration. Hao Zhang 1 , David J. Srolovitz 1,2 1 Princeton University 2 Yeshiva University. Z. v(y). Curvature-driven Grain Boundary Migration. U-shaped half loop geometry.

denis
Télécharger la présentation

Atomistic Mechanisms for Grain Boundary Migration

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Atomistic Mechanisms for Grain Boundary Migration  Overview of Atomistic Simulations of Grain Boundary Migration Hao Zhang 1, David J. Srolovitz 1,2 1 Princeton University 2 Yeshiva University

  2. Z v(y) Curvature-driven Grain Boundary Migration • U-shaped half loop geometry • Local Velocity • FCC Aluminum <111> Tilt Grain Boundary • EAM – Al • Periodic along X and Z • Steady-state Velocity

  3. Reduced Mobility vs. Misorientation • Reduced mobility increases with increasing temperature • Mobility shows maxima at low Σ misorientations

  4. 11 22 33 Free Surface 22 11 q 33 Grain 2 Z Grain Boundary X Grain 1 Y Free Surface Stress-Driven Boundary Migration • Molecular dynamics in NVT ensemble • EAM-type (Voter-Chen) potential for Ni • Periodic boundary conditions in x and y • One grain boundary & two free surfaces • Fixed biaxial strain,  =xx=yy • Source of driving force is the elastic energy • difference due to crystal anisotropy • Driving force is constant during simulation • Linear elasticity: • At large strains, deviations from linearity occur, • determine driving force from the difference of the strain energy in the 2 grains: S5 (001) tilt boundary

  5. Steady State Grain Boundary Migration

  6. a a Symmetric boundary Asymmetric boundary a = 14.04º Asymmetric boundary a = 26.57º Bicrystal Geometry [010] S5 36.87º

  7. Mobility vs. Inclination • No mobility data available at a=0, 45º; zero driving force • Mobilities vary by a factor of 4 over the range of inclinations studied at lowest temperature • Variation increases when temperature ↓ (from ~2 to ~4) • Minima in mobility occur where one of the boundary planes has low Miller indices H. Zhang et al.Scripta Materialia, 52: 1193; 2005

  8. Mobility, Diffusivity & Energy • At low T, self-diffusivity & grain boundary energy increase with increasing inclination • Mobility, self-diffusion coefficient and grain boundary energy exhibit local minimum at special inclination (at least one low index boundary plane) • All three quantities are correlated for a >18º M. Mendelev et al.JMR, 20: 1146; 2005

  9. Cahn & Taylor’s Model (2004) pure sliding initial pure shear combination • Boundary migration can also produce a coupled tangential motion of the two crystals relative to each other • In the absence of grain boundary sliding, the velocity parallel to the grain boundary, v||, is proportional to the grain boundary migration velocity, vn. The coefficient b is independent of grain boundary inclination. • Coupling coefficient b:

  10. v|| Suzuki & Mishin’s Simulation (2005) • [001] Symmetric tilt boundaries • Fix the bottom and shear the top with v|| = 1m/s • Grain boundary migrates ↑ or ↓

  11. v||=1m/s Shear (coupled) Motion - Symmetric Boundary • S5 [010] symmetric tilt boundary (103) at 800K • The step height = 1.11Ǻ ((103) plane spacing is 1.13Ǻ), therefore, the migration is plane by plane • Both Ashby and Cahn give the correct prediction for symmetric grain boundary

  12. Critical Stress for Shear (coupled) Motion • When the shear strain of lower grain reaches ~0.4%, migration was ignited. • The average critical stress is ~0.64 GPa. • This migration is difussionless

  13. Atomistic Migration Detail • 12: Atomic configurations apart by ~122 ps • The displacements represent elastic deformation; no indication of grain boundary sliding.

  14. Atomistic Migration Detail (Cont’d) • 23: Atomic configurations apart by 5.6 ps • Coupled sliding and migration  shear • Grain boundary migrates from blue line to red line • Top crystal uniformly slides right – releases elastic strain

  15. Atomistic Jump Picture (23)

  16. v|| v|| v|| Macroscopic Migration Picture (Symmetric) 3 2 1 12: Elastic deformation, Stress ↑ 23: Reach critical stress, two grains slide relatively to each other; stress release; boundary migrates Fixed ratio of migration/sliding shear

  17. a=18.43º a=9.46º a=26.57º a=36.87º Shear Motion in Asymmetric Boundaries T=500K, v||=0.5m/s

  18. Coupled motion at different T (a = 13.6º)

  19. Shear/coupled motion in General GB

  20. Critical Stresses

More Related