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CsCl can be thought of as two interpenetrating simple cubic arrays where the corner of one cell sits at the body center of the other. As with NaCl, the 1:1 stoichiometry means that the cell will look the same regardless of whether we start with anions or cations on the corner. Note that each ion is 8-coordinate rather than 6-coordinate as in NaCl.
| CsCl Vital Statistics | |
|---|---|
| Formula | CsCl |
| Crystal System | Cubic |
| Lattice Type | Primitive |
| Space Group | Pm3m, No. 221 |
| Cell Parameters | a = 4.123 Å, Z=1 |
| Atomic Positions | Cl: 0, 0, 0 Cs: 0.5, 0.5, 0.5 (can interchange if desired) |
| Density | 3.99 |
| Melting Point | 646 degrees C |
| Alternate Names | none |
| Isostructural Compounds |
NH4X, TlX (X = halide), CuZn (beta-brass), AgZn, LiHg, MgSr |
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| Fig. 1 A single unit cell of CsCl | Fig. 2 A 3x3x3 lattice of CsCl |
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| Fig. 3 The (111) plane of CsCl. | Fig. 4 The (100 plane of CsCl. |
Self-Study: Which set of planes contain the body center and the points (0,0,1), (1/2,0,1/2) and (0,1/2,1/2)?
Self-Study: What would a polyhedral representation of this structure look like?
| Fig. 5 A single unit cell of CsCl. | Fig. 6 A 2x2x2 chunk of CsCl lattice. |

This page was last updated Saturday, January 17, 2004
This document and associated figures are copyright 1996-2013 by Rob Toreki. All rights reserved.