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Callister - An introduction - 8th edition

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7.4 Slip Systems • 203<br />

D<br />

B<br />

A<br />

(a)<br />

E<br />

C<br />

F<br />

D<br />

B<br />

A<br />

E<br />

(b)<br />

C<br />

F<br />

Figure 7.6 (a) A {111}<br />

H110I slip system shown<br />

within an FCC unit cell.<br />

(b) The (111) plane<br />

from (a) and three<br />

H110I slip directions (as<br />

indicated by arrows)<br />

within that plane<br />

constitute possible slip<br />

systems.<br />

minimum. For a particular crystal structure, the slip plane is the plane that has the<br />

most dense atomic packing—that is, has the greatest planar density. The slip direction<br />

corresponds to the direction, in this plane, that is most closely packed with<br />

atoms—that is, has the highest linear density. Planar and linear atomic densities<br />

were discussed in Section 3.11.<br />

Consider, for example, the FCC crystal structure, a unit cell of which is shown<br />

in Figure 7.6a. There is a set of planes, the {111} family, all of which are closely<br />

packed. A (111)-type plane is indicated in the unit cell; in Figure 7.6b, this plane is<br />

positioned within the plane of the page, in which atoms are now represented as<br />

touching nearest neighbors.<br />

Slip occurs along H110I-type directions within the {111} planes, as indicated by<br />

arrows in Figure 7.6. Hence, 51116H110I represents the slip plane and direction combination,<br />

or the slip system for FCC. Figure 7.6b demonstrates that a given slip plane<br />

may contain more than a single slip direction. Thus, several slip systems may exist<br />

for a particular crystal structure; the number of independent slip systems represents<br />

the different possible combinations of slip planes and directions. For example, for<br />

face-centered cubic, there are 12 slip systems: four unique {111} planes and, within<br />

each plane, three independent H110I directions.<br />

The possible slip systems for BCC and HCP crystal structures are listed in Table<br />

7.1. For each of these structures, slip is possible on more than one family of planes<br />

(e.g., {110}, {211}, and {321} for BCC). For metals having these two crystal structures,<br />

some slip systems are often operable only at elevated temperatures.<br />

Table 7.1<br />

Slip Systems for Face-Centered Cubic, Body-Centered Cubic, and<br />

Hexagonal Close-Packed Metals<br />

Number of<br />

Metals Slip Plane Slip Direction Slip Systems<br />

Face-Centered Cubic<br />

Cu, Al, Ni, Ag, Au 51116 81109<br />

12<br />

Body-Centered Cubic<br />

a-Fe, W, Mo 51106 81119<br />

12<br />

a-Fe,W 52116 81119<br />

12<br />

a-Fe, K 53216 81119<br />

24<br />

Hexagonal Close-Packed<br />

Cd, Zn, Mg, Ti, Be 500016 811209<br />

3<br />

Ti, Mg, Zr 510106<br />

811209<br />

3<br />

Ti, Mg 510116<br />

811209<br />

6

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