Modeling Static Recrystallization in Al-Mg Alloys
ORIGINAL RESEARCH ARTICLE
Modeling Static Recrystallization in Al-Mg Alloys
HEINRICH BUKEN and ERNST KOZESCHNIK
In the present work, the influence of Mg on recrystallization kinetics in Al is analyzed by
computer simulation. A comprehensive state parameter-based microstructure model is
developed, which describes recrystallization in terms of nucleation and growth. The mechanism
of solute drag is fully incorporated, thus accounting for the decrease of grain boundary mobility
in the presence of impurity atoms. On the basis of the present approach, the solute binding
energy between Mg atoms and grain boundaries is assessed and compared to experimentally
measured values. Furthermore, the influence of Mg on dislocation production during strain
hardening is modeled. The simulations of the composition and temperature-dependent
recrystallization kinetics are verified on experimental studies where excellent agreement is
achieved. Both simulation and experiment show that increasing Mg content first decelerates
and, later on, accelerates recrystallization kinetics.
https://doi.org/10.1007/s11661-020-06100-9
Ó The Author(s) 2020
I.
INTRODUCTION
THE control of microstructure evolution during
processing of Mg-alloyed Al materials is a key factor
for determining the final mechanical–technological
properties of the material. Mg is a widely used element
in Al alloys, especially in the 5xxx and 6xxx series. On
the one hand, Mg segregates into grain boundaries and
reduces the mobility of the moving boundary by several
orders of magnitude in comparison to pure Al.[1] This
so-called solute drag effect[2] is caused by solute atoms
being dragged along with the moving grain boundary,
thus exerting a restraining force against the movement
of the grain boundary. As a result, microstructural
processes involving the motion of high-angle grain
boundaries (HAGB) and low-angle grain boundaries
(LAGB) can be severely slowed down by the presence of
impurity atoms.[1,3] On the other hand, an increased Mg
content promotes a higher strain-hardening rate, which,
at identical strain, induces a higher dislocation density.[4,5] As a result, the driving pressure for recrystallization increases, thus accelerating the observed
recrystallization kinetics. Koizumi et al.[6] have performed recrystallization experiments in Al-Mg alloys,
observing that an increase of the Mg content first leads
HEINRICH BUKEN is with the Primetals Technologies Austria
GmbH, Turmstrasse 44, 4031 Linz, Austria and also with the Institute
of Materials Science and Technology, TU Wien, Getreidemarkt 9,
1060 Vienna, Austria. ERNST KOZESCHNIK is with the Institute of
Materials Science and Technology, TU Wien and also with the
MatCalc Engineering GmbH, Getreidemarkt 9, 1060 Vienna, Austria.
Contact e-mail:
Manuscript submitted August 21, 2020; accepted November 6,
2020.
METALLURGICAL AND MATERIALS TRANSACTIONS A
to a deceleration of the rate of recrystallization, followed
by an acceleration at further increasing Mg content.
These results will form the basis of experimental
verification of the present model.
In literature, several approaches are available describing recrystallization phenomena in metallic materials.
With particular focus on Al alloys, earlier models[7,8]
mostly utilize JMAK-based equations[9] for describing
the kinetics of static recrystallization. In these models,
several semi-empirical parameters are commonly utilized to adjust the simulated recrystallizing kinetics to
experimentally measured recrystallized fractions. Since
JMAK-based models do not incorporate explicit mechanism-based descriptions for nucleation and growth of
recrystallizing grains, they can only take limited account
of basic physical phenomena such as the solute drag
effect, precipitate–dislocation interactions in precipitation hardening alloys or the influence of impurities on
dislocation generation during strain hardening.
Recently, Zurob et al.[10,11] presented a physically
based model describing recrystallization with explicit
expressions for nucleation and growth. In their work,
the nucleation rate for recrystallization is evaluated
from microstructural state parameters such as the
subgrain size and the dislocation density, which, in
combination with growth equations, delivers information on the recrystallized fraction within the deformed
microstructure. The solute drag impact is included in the
grain boundary mobility within the Cahn approach.[2]
When applying the model to Al, however, Zurob
et al.[10] utilized experimentally determined mobilities
taken from literature instead of calculating composition-dependent mobilities based on physical relationships. Furthermore, this work does not take into
account that the alloy composition has an important
impact on the dislocation evolution during and after
deformation. Consequently, no variation in the alloy
composition of various Al alloys is elaborated in this
work and recrystallization kinetics is evaluated only for
a single Mg content of 1 wt pct.
In the present work, a state parameter-based model is
developed, in which all relevant microstructural parameters are numerically integrated forward in time. The
evolution equations incorporate full composition and
temperature dependence for grain boundary mobilities
as well as dislocation generation during strain hardening. The calculated grain boundary mobilities are
compared to experimentally measured values to illustrate the predictive potential of the present grain
boundary mobility approach. In addition, relations, by
which the driving pressure for recrystallization is
described as a function of the Mg content through a
composition-dependent dislocation generation term, are
introduced. Furthermore, the previous version of the
model, which has been reported in References 12 and 13
is substantially improved in terms of the introduction of
the Rayleigh distribution for the rate of supercritical
subgrain formation (Section II–A) instead of a sharp
limit corresponding to the comparison of the mean and
critical subgrain sizes, as well as a dynamic treatment of
the subgrain size with growth and shrinkage terms
(Section II–B). The predictions of the recrystallization
model are finally compared with experimentally measured values from literature. The entire model and input
parameters are explained in detail, subsequently.
II.
THE RECRYSTALLIZATION MODEL
A. Nucleation and Growth
The nucleation rate of newly formed recrystallized
grains, N_ rx , is formulated as the product of the number
density of potential nucleation sites, Npot , a site saturation factor, Bnuc , which accounts for the grain area that
is already covered by recrystallized grains and which is,
therefore, no longer available for further nucleation, as
well as the flux of subgrains reaching supercritical size,
F_ sub , as
N_ rx ¼ Npot Bnuc F_ sub :
½1
Bailey and Hirsch[14] suggested that the main nucleation mechanism for recrystallization is given by the
process of strain-induced boundary migrat (...truncated)