Applied Surface Science 363 (2016) 543–547
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Applied Surface Science
jou rn al h om ep age: www.elsevier.com/locate/apsusc
Formation of core–shell structure in high entropy alloy coating by
laser cladding
Hui Zhang
a
, Wanfei Wu
a
, Yizhu He
a,∗
, Mingxi Li
a
, Sheng Guo
b,∗
a
School of Materials Science and Engineering, Anhui University of Technology, Ma’anshan, Anhui 243002, PR China
b
Surface and Microstructure Engineering Group, Department of Materials and Manufacturing Technology, Chalmers University of Technology, Gothenburg
SE-41296, Sweden
a r t i c l e i n f o
Article history:
Received 12 October 2015
Received in revised form
28 November 2015
Accepted 7 December 2015
Available online 12 December 2015
Keywords:
Liquid phase separation
High-entropy alloy
Laser cladding
Inoculant
a b s t r a c t
The formation of core–shell structure is an interesting phenomenon occurring during the solidification
process, due to the liquid phase separation. The formation of core–shell structure in high-entropy alloys,
a new class of advanced metallic materials, has not been reported previously, and thus constitutes an
intriguing scientific question. Here, we firstly report the formation of core–shell structure in one laser
cladded high-entropy alloy, where we show the nanosized-Y
2
O
3
powder addition, serves as the catalyst
for the liquid phase separation.
© 2015 Published by Elsevier B.V.
1. Introduction
The core–shell structure, occurring during the macroscopic
liquid phase separation, constitutes one of the most interesting
solidification microstructures [1]. The opportunity to create such
a special regular microstructure draws attention from researchers
in the field of condensed matter and materials physics. Liquid
phase separation usually takes place in immiscible alloys with a
large positive enthalpy of mixing [2]. However, it is usually diffi-
cult to achieve a high undercooling in these kinds of alloys, due
to the low liquid–liquid interface energy [2]. For example, in the
Cu–Co binary alloys, the metastable liquid phase separation only
occurs when a critical undercooling (50–80 K) is reached [3]. A
high undercooling can be achieved by melt processing methods,
including container-less solidification (typically electromagnetic
or electrostatic levitation, drop tube, and atomization) and
fluxing [3].
High-entropy alloys (HEAs), or multi-component alloy with
equi- or close to equiatomic compositions, are emerging novel
metallic materials with many interesting structural and func-
tional properties [4–7]. Investigations on the solidification behavior
∗
Corresponding author.
E-mail addresses: heyizhu@ahut.edu.cn (Y. He), sheng.guo@chalmers.se
(S. Guo).
(including liquid phase separation) of HEAs, as a kind of new
materials, can greatly enrich our understanding to the solidifi-
cation of multi-component alloys [8,9]. Interestingly, there has
so far no a single report on the formation of the core–shell
structure in HEAs, although the segregation involving Cu (Cu-
rich liquid solidifies later in the inter-dendritic region, after the
dendrites are solidified), which has positive enthalpy of mixing
with many alloying elements in HEAs [10], is commonly seen.
In addition, it has been shown that a large undercooling is not
necessarily leading to the formation of liquid phase separation
in HEAs. For example, Munitz et al. did not observe the liq-
uid phase separation in a Cu-rich HEA, Al
1.8
CoCrCu
3.5
FeNi, even
when the undercooling reached 150 K. They reckoned that an even
higher undercooling is required for the liquid phase separation to
occur.
The intention of the current work is to explore the pos-
sibility of forming the core–shell structure in HEAs, using
simultaneously two strategies. Firstly, we will use the laser
cladding method to achieve the high cooling rate, which will
also promote the high undercooling [3]. Secondly and more
importantly, we plan to use high melting point nanosized par-
ticles as inoculants, to catalyze the liquid phase separation
. Our idea is inspired by the promotion of liquid phase separation by
the addition of Al
2
O
3
, ZrO
2
and TiB
2
to Al–Bi and Al–Pb monotectic
binary alloys [11,12]. As will be shown later, the addition of inoc-
ulants indeed proved to be the key. To the best of our knowledge,
http://dx.doi.org/10.1016/j.apsusc.2015.12.059
0169-4332/© 2015 Published by Elsevier B.V.