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Chapter 2<br />

Basic Structural Concepts<br />

A Introduction<br />

Crystal structures have already been mentioned and a few simple diagrams<br />

(Figs. 1.7a, 1.13, and 1.14c, for example) were presented in the last chapter. To<br />

understand crystal structures in a systematic way, one must be familiar with the<br />

formal methods of describing them. The objective of this chapter is to begin to<br />

explain how crystal structures are described and classified. The most important<br />

topics in this chapter are the definition of the lattice (both direct and reciprocal),<br />

the description of techniques for quantifying lattice components (directions<br />

and planes), and the idea that every structure can be described as a<br />

combination of a lattice and a basis. This chapter also includes a description of<br />

how crystal structures are visually represented and an introduction to polycrystallography.<br />

B The Bravais lattice<br />

The Bravais lattice is the periodic array in which the repeated units of the crystal<br />

are arranged. Because there are only 14 distinct arrangements, the Bravais lattice<br />

system provides a convenient mechanism for classifying the structural diversity<br />

that occurs in nature. However, one must remember that the Bravais lattice<br />

describes only the underlying configuration of the repeat units. It says nothing<br />

about the arrangement of atoms within the repeat unit. In this case, specificity is<br />

sacrificed for simplicity.<br />

i. Definition<br />

A good definition of a Bravais lattice is that it is an infinite array of discrete<br />

points with an arrangement and orientation that appears exactly the same<br />

regardless of the point from which the array is viewed. A more practical quantitative<br />

definition is that a Bravais lattice consists of all points defined by position<br />

vectors, R, of the form:<br />

Ruavbwc (2.1)<br />

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