Materials Science Forum
Vol. 570
Vol. 570
Materials Science Forum
Vol. 569
Vol. 569
Materials Science Forum
Vols. 567-568
Vols. 567-568
Materials Science Forum
Vol. 566
Vol. 566
Materials Science Forum
Vols. 561-565
Vols. 561-565
Materials Science Forum
Vol. 560
Vol. 560
Materials Science Forum
Vols. 558-559
Vols. 558-559
Materials Science Forum
Vols. 556-557
Vols. 556-557
Materials Science Forum
Vol. 555
Vol. 555
Materials Science Forum
Vol. 554
Vol. 554
Materials Science Forum
Vol. 553
Vol. 553
Materials Science Forum
Vols. 551-552
Vols. 551-552
Materials Science Forum
Vol. 550
Vol. 550
Materials Science Forum Vols. 558-559
Paper Title Page
Abstract: The development of a digital material framework is presented, allowing to build virtual
microstructures in agreement with experimental data. The construction of the virtual material
consists in building a multi-level Voronoï tessellation. A polycrystalline microstructure made of
grains and sub-grains can be obtained in a random or deterministic way. A corresponding finite
element mesh can be generated automatically in 3D, and used for the simulation of mechanical
testing under large strain. In the examples shown in this work, the initial mesh was non uniform and
anisotropic, taking into account the presence of interfaces between grains and sub-grains. Automatic
remeshing was performed due to the large strains, and maintained the non uniform and anisotropic
character of the mesh. A level set approach was used to follow the grain boundaries during the
deformation. The grain constitutive law was either a viscoplastic power law, or a crystallographic
formulation based on crystal plasticity. Stored energies and precise grain boundary network
geometries were obtained directly from the deformed digital sample. This information was used for
subsequent modelling of grain growth with the level set approach, on the same mesh.
1133
Abstract: The classical JMAK equation was modified by combination with distribution density of
the rate parameter k, which was deduced from a normal distribution of local strain. The modified
equation is able to calculate the JMAK plots and the average Avrami exponent to characterize the
entire heterogeneous recrystallization process. This new extension can successfully describe the
relevant experimental observations, such as a smaller exponent than the basic JMAK theory
predicts, and a decreasing slope of JMAK plots with the proceeding recrystallization. Moreover, it
reveals that the Avrami exponent observed experimentally should significantly decrease with the
increasing standard deviation of local strain distribution. In addition, it has a great potential to
explain why most of experimentally observed values of Avrami exponents are less than 2 and why
the Avrami exponent is insensitive to temperature and deformation conditions when the real
standard deviation of local strain distribution in deformed metals is known.
1139
Abstract: The competitive behaviors between recrystallization and transformation during annealing
in dual phase high-strength steels are studied both by experiments and by computer simulations. The
Monte Carlo code was applied to simulate such competing behavior, explained the experimental
results, as follows. (1) The progress of the transformation is affected by the starting point of the
transformation in the course of recrystallization. Namely, if the transformation starts at the later stage
of recrystallization, the n-value in JMAK equation is relatively high. (2) If the stored energy (driving
force) of the transformation is above 5 times larger than that of the recrystallization, the effect of the
stored energy is quite small. (3) If the number of nuclei were increased, the transformation proceeds a
little faster, and then the transformed microstructures are significantly refined. When the
transformation initiates at the early stage of the recrystallization, the number of nuclei can be
increased by nucleation from the deformed matrix compared with the one from fully recrystallized
matrix.
1145
Abstract: The generalized deterministic vertex model was successfully used to study the
recrystallization process and the corresponding results were published elsewhere [1]. In its classical
form the vertex model has analytical formulation, basing on the total energy (i.e. boundary energy
and stored energy) minimization. A change of grain boundary configuration in classical vertex
model is found by the calculation of vertex velocities. Consequently, a global and complex system
of equations has to be solved in each step.
In order to simplify calculations and to handle the problem in a more flexible way, the statistical
model was proposed. Typical elements of Monte Carlo algorithm were incorporated into the vertex
model: a random (and small) modification of microstructure is accepted with the probability
proportional to Boltzmann factor. This approach is closer to the stochastic nature of recrystallization
process. The model was used to study the recrystallization of 70% and 90% cold rolled
polycrystalline copper. It predicts correctly recrystallization textures for high and low strains.
1151
Abstract: Classical vertex model till now described only the grain growth stage and not the primary
recrystallization. In the present work the vertex model is first extended in order to take into account
the both stages of recrystallization process. The influence of the stored energy is taken into account
and some phenomenological laws describing the evolution of grain boundary energy and mobility
with misorientation angle are used. Nucleation is considered to be site-saturated. The
experimentally determined stored energy values, crystallographic orientations and boundary
misorientation distributions are used in order to characterize the initial microstructure. The model is
tested to study the recrystallization of 70% and 90% cold rolled polycrystalline copper during an
annealing treatment. In order to explain the texture evolution in both cases, it is necessary to
introduce an energy threshold for grain boundary movement, i.e. a minimal value of the stored
energy difference between a nucleus and the deformed material necessary to provoke grain
boundary motion. The developed model is shown to predict texture evolutions in good agreement
with experimental data.
1157
Abstract: A 2D cellular automaton model developed for the simulation of grain growth in
hexagonal metals is presented here. It allows the direct use of experimental measurement as input
data. Texture evolution of a titanium alloy and a zirconium alloy are simulated on the basis of
simple hypothesis and compared with experimental evolution as well as the results from a 3D
Monte Carlo model. Results from both models are discussed with regards to their characteristics.
1163
Abstract: A refined view of particle stimulated nucleation of recrystallization is presented, which
utilizes a combination of advanced modeling tools. FEM simulations were carried out in order to
model the evolution of the deformation zone around particles for various particle sizes and shapes.
The results of these simulations were complemented by EBSD measurements to determine the
number and orientation of nuclei. Finally, this information on particle stimulated nucleation was
incorporated into a 3D cellular automaton recrystallization model CORe to model microstructure
evolution. From these simulations the dependence of grain size and texture on particles size and
shape was derived.
1169
Abstract: The kinetics and topology of ideal grain growth were simulated using the phase-field
model. Large scale phase-field simulations were carried out where ten thousands grains evolved into
a few hundreds without allowing coalescence of grains. The implementation was first validated in
two-dimensions by checking the conformance with square-root evolution of the average grain size
and the von Neumann-Mullins law. Afterwards three-dimensional simulations were performed
which also showed fair agreement with the law describing the evolution of the mean grain size
against time and with the results of S. Hilgenfeld et al. in 'An Accurate von Neumann's Law for
Three-Dimensional Foams', Phys. Rev. Letters, 86(12)/2685, March 2001. Finally the steady state
grain size distribution was investigated and compared to the Hillert theory.
1177
Abstract: Based on topological considerations and results of Monte Carlo Potts model simulations
of three-dimensional normal grain growth it is shown that, contrary to Hillert’s assumption, the
average self-similar volume change rate is a non-linear function of the relative grain size, which in
the range of observed grain sizes can be approximated by a quadratic polynomial. In particular,
based on an adequate modification of the effective growth law, a new analytical grain size
distribution function is derived, which yields an excellent representation of the simulated grain size
distribution.
1183
Abstract: The effects of second-phase particles on the recrystallization kinetics in two-dimensional
polycrystalline structures were investigated. Numerical simulations of recrystallization were
performed by coupling the unified subgrain growth theory with a phase-field methodology. Simple
assumptions based on experimental observations were utilized for preparing initial microstructures.
The following results were obtained: (1) The presence of second-phase particles retarded
recrystallization speeds. (2) If the mean subgrain size was small enough recrystallized region covered
whole system for various values of the particle fraction, f. (3) On the other hand, if the mean subgrain
size was not small enough the progress of recrystallization was frozen at some point.
1189