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D GENERALIZATIONS ABOUT CRYSTAL STRUCTURES BASED ON PERIODICITY<br />

Figure 1.8. Geometric configurations with different radius ratios. (a) shows a stable configuration.<br />

The ions in (b) have the minimum radius ratio for stability in this arrangement. The<br />

radius ratio of the ions in (c) makes this an unstable configuration.<br />

Stable and unstable configurations are illustrated in Fig. 1.8. Basically, a configuration<br />

is stable until anion–anion repulsions force longer and less stable<br />

anion–cation bond distances (as in 1.8c). The critical or minimum stable radius<br />

ratio is defined by the point when the cation contacts all of the neighboring<br />

anions, and the anions just contact one another, as shown in Fig. 1.8(b). For any<br />

given coordination number, there is a minimum stable radius ratio that can be<br />

derived through simple geometric arguments (see Example 1.2). Atoms with<br />

radius ratios as shown in 1.8(c) would be more stable in a configuration with a<br />

lower coordination number. The minimum radius ratios for selected geometries<br />

are summarized in Fig. 1.10.<br />

Example 1.2 Calculating minimum stable radius ratios<br />

Determine the minimum stable radius ratio for octahedral (six-fold)<br />

coordination.<br />

1. First, assume that the cation in the center contacts the surrounding anions and that<br />

the anions just contact one another (this is the minimum stable configuration). Using<br />

Fig. 1.9, we find a plane that contains both cation–anion and anion–anion contacts.<br />

One such plane is the equatorial plane (see Fig. 1.9b).<br />

2. Next, we note that the sides of the isosceles triangles in Fig. 1.9 have the lengths:<br />

abr and cr r . Based on these geometric relationships, the radius ratio can<br />

be easily determined:<br />

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