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Callister - An introduction - 8th edition

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3.10 Crystallographic Planes • 63<br />

z axes are a, a, and c, respectively. First we begin at the origin (point O),<br />

then proceed a units along the a 1 axis (to point P), next parallel to the a 2<br />

axis a units (to point Q), and finally parallel to the z axis c units (to point<br />

R). Hence, the [111] direction is represented by the vector that passes from<br />

O to R as shown.<br />

It may be noted that this [111] direction is identical to [1123] from part (b).<br />

The alternative situation is to determine the indices for a direction that has been<br />

drawn within a hexagonal unit cell. For this case it is convenient to use the a 1 -a 2 -z<br />

three-coordinate-axis system and then convert these indices into the equivalent set for<br />

the four-axis scheme. The following example problem demonstrates this procedure.<br />

EXAMPLE PROBLEM 3.9<br />

Determination of Directional Indices for a Hexagonal<br />

Unit Cell<br />

Determine the directional indices (four-index system) for the direction shown<br />

in the accompanying figure.<br />

z<br />

Projection on z<br />

axis (c/2)<br />

a 2<br />

c<br />

a<br />

a<br />

a 1<br />

Projection on a 2<br />

axis (–a)<br />

Solution<br />

The first thing we need do is to determine indices for the vector referenced<br />

to the three-axis scheme represented in the sketch. Because the direction vector<br />

passes through the origin of the coordinate system, no translation is necessary.<br />

Projections of this vector onto the a 1 , a 2 , and z axes are 0a, a, and c2,<br />

1<br />

respectively, which become 0, 1, and 2 in terms of the unit cell parameters.<br />

Reduction of these numbers to the lowest set of integers is possible by<br />

multiplying each by the factor 2. This yields 0, 2, and 1, which are then enclosed<br />

in brackets as [ 021].

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