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Introduction to Nanotechnology

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140 BULK NANOSTRUCTURED MATERIALS<br />

where B, is the fhctional stress opposing dislocation movement, K is a constant, and<br />

d is the grain size in micrometers. Hardness can also be described by a similar<br />

equation. Figure 6.9 plots the measured yield strength of Fe-Co alloys as a function<br />

of d-(’’’), showing the linear behavior predicted by Eq. (6.1). Assuming that the<br />

equation is valid for nanosized grains, a bulk material having a 50-nm grain size<br />

would have a yield strength of 4.14 GPa. The reason for the increase in yield strength<br />

with smaller grain size is that materials having smaller grains have more grain<br />

boundaries, blocking dislocation movement. Deviations from the Hall-Petch beha-<br />

vior have been observed for materials made of particles less than 20 nm in size. The<br />

deviations involve no dependence on particle size (zero slope) <strong>to</strong> decreases in<br />

yield strength with particle size (negative slope). It is believed that conventional<br />

dislocation-based deformation is not possible in bulk nanostructured materials with<br />

sizes less than 30 nm because mobile dislocations are unlikely <strong>to</strong> occur. Examination<br />

of small-grained bulk nanomaterials by transmission electron microscopy during<br />

deformation does not show any evidence for mobile dislocations.<br />

Most bulk nanostmctured materials are quite brittle and display reduced ductility<br />

under tension, typically having elongations of a few percent for grain sizes less than<br />

30 nm. For example, conventional coarse-grained annealed polycrystalline copper is<br />

very ductile, having elongations of up <strong>to</strong> 60%. Measurements in samples with grain<br />

sizes less than 30nm yield elongations no more than 5%. Most of these measure-<br />

ments have been performed on consolidated particulate samples, which have large<br />

residual stress, and flaws due <strong>to</strong> imperfect particle bonding, which restricts disloca-<br />

1300~1 I I I I I I I I I I I I I 1 I I I I I I I I 14<br />

1//d (microns)-’’2<br />

Figure 6.9. Yield strength of Fe-Co alloys versus l/d’/‘, where d is the size of the grain.<br />

[Adapted from C.-H. Shang et al., J. Mater. Res. 15, 835 (2000).]

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