DOI: 10.1002/adem.201400423
Strain Gradient in Micro-Hardness Testing and Structural
Relaxation in Metallic Glasses**
By Yannick Champion* and Lo € ıcPerrie`re
An analytical model is proposed to quantitatively describe the depth-dependence of Vickers micro-
hardness in metallic glasses. The approach is based on a shear bands distribution-induced strain
gradient during testing and was used to analyze thermal relaxation in the Zr
55
Cu
20
Al
10
Ni
10
Ti
5
,
Ni
53
Nb
20
Zr
8
Ti
10
Co
6
Cu
3
, and Mg
65
Cu
12.5
Ni
12.5
MM
10
metallic glasses. It was shown that a decrease of
the free volume leads systematically to a decrease of the alloy hardness. This analysis also gives an
evaluation of the shear band thickness and the role of the elastic properties in the depth-dependence of
the Vickers micro-hardness.
1. Introduction
Indentation testing is providing with a preliminary insight
of the mechanical properties of materials (strength, ductile/
fragile character, and toughness).
[1,2]
For example, it allows to
follow easily the mechanical behavior evolutions during
processing of a material and then gives a semi-quantitative
guideline for its preparation and optimization. Among the
various techniques, the Vickers indentation is probing at
micrometer range length scale, which is well suited for
investigations in materials science. For example, the strength
s
s
is simply derived according to the Tabor rule: H ¼ 2.8
s
s
(0.15)
n
, with H, the Vickers hardness and n the work-
hardening coefficient.
A specific feature of indentation is the dependence of the
measurement with the indent size or indent depth.
[3]
This is
quantitatively explained for crystalline solids based on the
dislocations theory. Ashby has proposed the general rule that
a non-symmetric plastic deformation (as in indentation where
deformation is confined) generates a strain gradient in the
deformation zone. It results an extra hardening that Ashby
described in terms of geometrically necessary dislocations
(GND).
[4]
Using this approach, Nix and Gao
[5]
showed that the
hardness measured follows the rule: H=H
0
¼
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
1 þ h
=h
p
, with
h* a constant depending on the materials and H
0
the hardness
at infinite indent size. For non-crystalline solids, the rule is
obviously different since dislocation are undefined. For
metallic glasses, the deformation is localized in thin shear
bands. This leads to absence of macroscopic plasticity when
they are tested in tension or compression, but the plasticity is
observed in indentation owing to the confined character of the
testing. Similar to crystalline solids a depth-dependence of the
hardness is observed,
[6]
but its follows a rule slightly different:
H=H
0
¼ 1 þ
ffiffiffiffiffiffiffiffiffi
h
=h
p
.
[7]
In this work, three different metallic glasses (Zr, Ni, and Mg
based) were studied using Vickers micro-hardness testing at
various loads to analyze the depth-dependence. In addition,
experiments were performed after various thermal treatments
in order to reveal the effect of structural relaxation on the
glasses properties. A quantitative analytical description of the
Vickers hardness variation with the indent size is then
proposed based on strain gradient induced by the shear bands
distribution and we show that this variation follows the
relation: H=H
0
¼ 1 þ
ffiffiffiffiffiffiffiffiffi
h
=h
p
. The modeling is used to analyze
thermal relaxation effects on the hardness and the elastic
properties of the Zr-, Ni-, and Mg-based metallic glass (MG)
alloys. The role of shear bands in the strain gradient induced
depth-dependence of the hardness is emphasized. As the
mode of plastic deformation in MG, shear banding analysis is
necessary for improving glass properties.
2. Experimental Section
Three MG alloys having different mechanical and thermal
properties have been investigated. A Zr-based MG
(Zr
55
Cu
20
Al
10
Ni
10
Ti
5
, with glass transition T
g
¼ 390 °C, strength
of 1.7 GPa, elastic modulus 80 GPa) characterized by a high
glass forming ability (GFA) was prepared by r.f. levitation
melting and quenching in a copper crucible into cylinder form
(diameter and length up to 10 and 30mm).
[8]
A Ni-based
(Ni
53
Nb
20
Zr
8
Ti
10
Co
6
Cu
3
, T
g
¼ 585 °C, strength about 2.7 GPa
[*] Y. Champion, L. Perrière
Institut de Chimie et des Mat eriaux Paris-Est, CNRS-UPEC, 2
rue Henri Dunant 94320, Thiais Cedex, France
E-mail: champion@icmpe.cnrs.fr
[**] This work was supported by the ANR and the French MoD
under the program ASTRID (2012–14) VMPB n° ANR-11-
ASTR-03601. Arnold Soppo and Yvan Cotrebil are gratefully
acknowledged for technical assistance.
DOI: 10.1002/adem.201400423 © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim wileyonlinelibrary.com 1
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