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Structural Investigation of Size Effects in Plasticity using Indentation ...

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1 Introduction<br />

changes with the depth <strong>of</strong> penetration. One type <strong>of</strong> <strong>in</strong>denter, which meets this geometric<br />

similarity, is the Vickers <strong>in</strong>denter. 5,6 Consequently, Meyer analysis <strong>of</strong> Vickers<br />

hardness data should yield a constant Meyer <strong>in</strong>dex <strong>of</strong> 2. In the follow<strong>in</strong>g many studies<br />

were performed us<strong>in</strong>g the Vickers hardness test and it was found that the Vickers<br />

hardness as well is load-dependent, especially at low loads. 6–9<br />

In the follow<strong>in</strong>g, great efforts were made to expla<strong>in</strong> the observed behavior. Generally,<br />

two sets <strong>of</strong> explanations can be dist<strong>in</strong>guished. The first set concerns experimental<br />

errors, 10 result<strong>in</strong>g from the resolution <strong>of</strong> the objective lens, 11,12 the geometry<br />

<strong>of</strong> the <strong>in</strong>denter, 13 friction between <strong>in</strong>denter and specimen 13–15 and errors associated<br />

with sample preparation. 7,8,16,17 The second set 1,18 is directly related to the <strong>in</strong>tr<strong>in</strong>sic<br />

structural factors <strong>of</strong> the tested materials, <strong>in</strong>clud<strong>in</strong>g e.g. <strong>in</strong>dentation elastic<br />

recovery 14,19–25 and work harden<strong>in</strong>g dur<strong>in</strong>g <strong>in</strong>dentation. 1 The conclusion was, that<br />

load-dependent hardness is a genu<strong>in</strong>e effect and is not caused by <strong>in</strong>strumental errors<br />

or the presence <strong>of</strong> a surface layer. A more detailed review on the early work <strong>of</strong><br />

load-dependent hardness can be found <strong>in</strong> the work <strong>of</strong> Mott. 1<br />

One <strong>of</strong> the first systematic <strong>in</strong>vestigations on load-dependency <strong>of</strong> hardness, was<br />

performed by Upit and Varchenya 26–29 on various s<strong>in</strong>gle crystall<strong>in</strong>e materials, us<strong>in</strong>g<br />

a low-load microhardness test<strong>in</strong>g device. Upit and Varchenya found that the<br />

<strong>in</strong>crease <strong>in</strong> hardness with decreas<strong>in</strong>g load, is associated with a correspond<strong>in</strong>g reduction<br />

<strong>of</strong> the size <strong>of</strong> dislocation assemblies, surround<strong>in</strong>g the <strong>in</strong>dentations. They<br />

called the observed variation <strong>of</strong> hardness with load, “size effect”. However, the term<br />

“<strong>in</strong>dentation size effect” (ISE) was accepted years later. At the same time, Gane<br />

and Cox 30,31 performed <strong>in</strong>dentation experiments on s<strong>in</strong>gle crystall<strong>in</strong>e gold. Gane<br />

and Cox found, that hardness could be <strong>in</strong>creased by a factor <strong>of</strong> three when decreas<strong>in</strong>g<br />

the contact diameter down to 200 nm. They suggested, that the <strong>in</strong>crease must<br />

have some fundamental orig<strong>in</strong>s, connected to dislocation processes occurr<strong>in</strong>g <strong>in</strong> the<br />

stressed volume around the <strong>in</strong>denter.<br />

More than one decade later, the development <strong>of</strong> <strong>in</strong>strumented nano<strong>in</strong>dentation<br />

techniques rek<strong>in</strong>dled the <strong>in</strong>terest <strong>in</strong> the phenomenon <strong>of</strong> load-dependent hardness.<br />

Instrumented <strong>in</strong>dentation technique was used by Pethica et al. 32 to perform hardness<br />

tests on nickel, gold and silicon us<strong>in</strong>g <strong>in</strong>denter penetration depths as low as<br />

20 nm. The <strong>in</strong>denter penetration was monitored cont<strong>in</strong>uously dur<strong>in</strong>g load<strong>in</strong>g and<br />

unload<strong>in</strong>g, while the areas <strong>of</strong> the <strong>in</strong>dents were determ<strong>in</strong>ed by means <strong>of</strong> a scann<strong>in</strong>g<br />

electron microscope (SEM). 33 For every material under exam<strong>in</strong>ation a pronounced<br />

<strong>in</strong>dentation size effect was found, especially for depths less than 100 nm. Pethica et<br />

al. expla<strong>in</strong>ed the <strong>in</strong>dentation size effect by local extreme work harden<strong>in</strong>g, s<strong>in</strong>ce all<br />

glide planes are active and <strong>in</strong>tersect<strong>in</strong>g <strong>in</strong> regions less than 100 nm across. 32<br />

Further improvement <strong>of</strong> <strong>in</strong>strumented nano<strong>in</strong>dentation technique was achieved<br />

by the work <strong>of</strong> Doerner and Nix 34 as well as Oliver and Pharr. 35 The enhanced<br />

technique made the determ<strong>in</strong>ation <strong>of</strong> mechanical properties from load-displacement<br />

curves possible, even when the <strong>in</strong>dentations were too small to be imaged conveniently.<br />

Driven by the grow<strong>in</strong>g <strong>in</strong>terest <strong>in</strong> the deformation <strong>of</strong> small material volumes<br />

caused by the development <strong>of</strong> th<strong>in</strong> films and the <strong>in</strong>creased use <strong>of</strong> nanostructured materials,<br />

load and displacement sens<strong>in</strong>g <strong>in</strong>dentation became a major tool to <strong>in</strong>vestigate<br />

2

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