Vol.:(0123456789) 1 3
Metals and Materials International
https://doi.org/10.1007/s12540-018-00225-8
Neural Network Approach to Construct a Processing Map
from a Non‑linear Stress–Temperature Relationship
Chan Hee Park
1
· Dojin Cha
2
· Minsoo Kim
2
· N. S. Reddy
3
· Jong‑Taek Yeom
1
Received: 24 October 2018 / Accepted: 20 November 2018
© The Korean Institute of Metals and Materials 2018
Abstract
An accurate processing map for a metal provides a means of attaining a desired microstructure and required shape through
thermo-mechanical processing. To construct such a map, the isothermal fow stress, σ
iso
, is required. Conventionally, the
non-isothermal fow stress measured by experiment is corrected to σ
iso
using whole-temperature-range linear interpolation
(WRLI) or partial-temperature-range linear interpolation (PRLI). However, these approaches could incur signifcant errors if
the non-isothermal fow stress exhibits a non-linear relationship with the temperature. In this study, an artifcial neural network
(ANN) model was applied to correct the non-isothermal fow stress in 10 wt% Cr steel, which exhibits a non-linear tempera-
ture dependence within a target temperature range of 750–1250 °C. Processing maps were constructed using σ
iso
corrected by
applying the WRLI, PRLI, and ANN approaches, respectively, and were then compared with the actual microstructures. The
WRLI approach produced the highest minimum error of σ
iso
(17.2%) and over-predicted the shear-band formation. The PRLI
approach reasonably predicted the microstructural changes, but the minimum error for σ
iso
(8.9%) was somewhat high. The ANN
approach not only realized the lowest minimum error of σ
iso
(~ 0%), but also efectively predicted the microstructural changes.
Keywords Metallic alloys · Thermomechanical · Processing · Microstructure · Stress–strain measurements · Computer
modelling
1 Introduction
A processing map is constructed by superimposing an
instability map [1–3] or fow localization map [4] onto a
power dissipation map [5]. The resulting processing map
can be employed to predict the microstructure evolution and
to optimize the thermo-mechanical processing of various
metals. Application of these theories requires a database of
isothermal fow stress σ
iso
as functions of strain, strain rate,
and target temperature T
target
. In most experiments, however,
the non-isothermal fow stress σ
non-iso
is obtained because
the instantaneous temperature T
instant
of the specimen dif-
fers from T
target
, especially in the case of high strain rates in
which deformation heating occurs. Thus, σ
non-iso
should be
corrected to σ
iso
prior to the construction of the processing
map.
There are many constitutive equations for determining
σ
iso
. These can be classifed into phenomenological models
and physically based models. The phenomenological mod-
els such as the Johnson–Cook (JC) [6], Khan–Huang–Liang
(KHL) [7, 8], and their modifcations [9, 10] always require
fow stress data at a low strain rate, at which deformation
heating does not occur, to identify material constants. Mean-
while, the physically based models, such as the mechanical
threshold stress (MTS) model [11, 12] and its modifca-
tions [13, 14], require fow stress values at either low or
very high temperatures to determine the threshold stress or
* Chan Hee Park
chpark@kims.re.kr
Dojin Cha
dojin.cha@doosan.com
Minsoo Kim
min-soo.kim@doosan.com
N. S. Reddy
nsreddy@gnu.ac.kr
Jong-Taek Yeom
yjt96@kims.re.kr
1
Advanced Metals Division, Korea Institute of Materials
Science, Changwon 51508, Republic of Korea
2
Corporate R&D Institute, Doosan Heavy Industries
and Construction, Changwon 51711, Republic of Korea
3
School of Materials Science and Engineering, Gyeongsang
National University, Jinju 52828, Republic of Korea