temperature dependence of grain boundary migration in 3-d hao zhang david j. srolovitz
DESCRIPTION
Temperature Dependence of Grain Boundary Migration in 3-D Hao Zhang David J. Srolovitz Princeton University Princeton Materials Institute (PMI). Acknowledgements Moneesh Upmanyu ORNL - PowerPoint PPT PresentationTRANSCRIPT
Temperature Dependence of Grain Boundary Migration in 3-D
Hao ZhangDavid J. SrolovitzPrinceton University
Princeton Materials Institute (PMI)
Acknowledgements
Moneesh Upmanyu ORNLLasar Shvindlerman Russian Academy of Sciences/RWTHGunther Gottstein RWTH AachenS. Srinivasan LANL
Outline
• Atomic Simulation Model
• Modeling Approach
• Driving Force Dependence of Migration
• Recent 3-D Results (Temperature Dependence)• Reduced Mobility• Grain Boundary Energy• Mobility• Activation Energy
• Conclusions
Grain boundary migration
• Absolute reaction rate theory (Turnbull, 1951)
• Grain growth (capillarity-induced migration)
)Tk
Q(MM
B
gbO expFMv gb
gbF )( gbgbMv
Grain Boundary Migration
• Local velocity
• Steady-state velocity
v(y)
• Boundary energy
t
A
tE
)2
w( g
gb
• U-shaped half loop geometry
][MMFv
Modeling Approach• FCC Aluminium <111> Tilt Grain Boundary
• EAM – Al
• Periodic along X, Y and Z
*Mww
Mv
w
Av
g
gA*MM
Driving Force Dependence of Migration
Driving Force /w (nm-1)M
igra
tion
rat
e v
(r
o/)
Red
uce
d M
obil
ity
Mgb
gb
(ao/
)
Gra
i n B
oun
dar
y E
ner
gy (
J/m
2 )For sufficiently low driving forces :
• Reduced mobility is independent of driving force (2-D)
• Migration rate is proportional to driving force (2-D)
• Grain Boundary Energy is large (3-D)
gbA
E
gA*MM
t
A
tE
)2
w( g
gb
7 Grain Boundary at T=427K
Grain Boundary Migration
M* vs. Misorientation
13 7(m
4/Js)
(deg)
13 7
Mobility and γ vs. Misorientation
t
A
tE
)2
w( gb
gb
gbA*MM
713
(J/m
2)
(m4/Js)
(deg) (deg)
Mobility vs. Misorientation
13 7(m
4/J
s)
(deg)
Simulation
Experiments
Temperature Dependence of Mobility
Activation Energy vs. Misorientation
experiment
Misorientation (deg)
Q (
e V)
Simulation 7
(eV
)
(deg)
• Reduced mobility shows local maxima at low 7
• Mobility shows maxima at low misorientations
• Boundary energy exhibits minima at low misorientations
• Magnitude of activation energy in simulation << than in
experiment
• Possible reasons: simulations do not represent the true physics
impurities
Conclusions