Coupling of a crystal plasticity finite-element model with a probabilisticcellular automaton for simulating primary static recrystallization in aluminium
D. Raabe et Rc. Becker, Coupling of a crystal plasticity finite-element model with a probabilisticcellular automaton for simulating primary static recrystallization in aluminium, MODEL SIM M, 8(4), 2000, pp. 445-462
The paper presents a two-dimensional approach for simulating primary static
recrystallization, which is based on coupling a viscoplastic crystal plast
icity finite-element model with a probabilistic kinetic cellular automaton.
The crystal plasticity finite-element model accounts for crystallographic
slip and for the rotation of the crystal lattice during plastic deformation
. The model uses space and time as independent variables and the crystal or
ientation and the accumulated slip as dependent variables. The ambiguity in
the selection of the active slip systems is avoided by using a viscoplasti
c formulation that assumes that the slip rate on a slip system is related t
o the resolved shear stress through a power-law relation. The equations are
cast in an updated Lagrangian framework. The model has been implemented as
a user subroutine in the commercial finite-element code Abaqus. The cellul
ar automaton uses a switching rule that is formulated as a probabilistic an
alogue of the Linearized symmetric Turnbull kinetic equation for the motion
of sharp grain boundaries. The actual decision about a switching event is
made using a simple sampling nonMetropolis Monte Carlo step. The automaton
uses space and rime as independent variables and the crystal orientation an
d a stored energy measure as dependent variables. The kinetics produced by
the switching algorithm are scaled through the mesh size, the grain boundar
y mobility, and the driving force data. The coupling of the two models is r
ealized by: translating the state variables used in the finite-element plas
ticity model into state variables used in the cellular automaton; mapping t
he finite-element integration point locations on the quadratic cellular aut
omaton mesh; using the resulting cell size, maximum driving force, and maxi
mum grain boundary mobility occurring in the region for determining the len
gth scale, time step, and local switching probabilities in the automaton; a
nd identifying an appropriate nucleation criterion. The coupling method is
applied to the two-dimensional simulation of texture and microstructure evo
lution in a heterogeneously deformed, high-purity aluminium polycrystal dur
ing static primary recrystallization, considering local grain boundary mobi
lities and driving forces.