The seven crystal systems Chemistry 4000/5000/6000 Chemical Crystallography The unit cells of the primitive lattices Trigonal vs. Hexagonal o o o This figure highlights the relationship between the rhombohedral primitive and the conventional hexagonal triple unitit cells ll for f the th trigonal ti l crystal t l system. It also illustrates the special character of “hexagonal” where the primitive unit cell is also one third of the full hexagon that describes the 6-fold rotation axis of hexagonal crystals. Why does the hexagonal triple of the trigonal system not have hexagonal, but instead trigonal (i.e. 3-fold rotation) symmetry? The hexagonal lattice o o o A hexagonal lattice can most easily be visualized in the ab plane This reduces the problem to 2 dimensions which is easier to visualize It is called hexagonal because of the six-fold axis described by the faint black lines y z x 1 The hexagonal lattice o o o o o o A hexagonal lattice can most easily be visualized in the ab plane This reduces the problem to 2 dimensions which is easier to visualize It is called hexagonal because of the six-fold axis described by the faint black lines BUT the hexagon is NOT the unit cell, which is given in red Th unitit cells The ll mustt stack t k together to give the entire lattice Hence the green lozenges represent the multiple unit cells The hexagonal lattice o o o y z x o o o o Trigonal vs. hexagonal lattices o o o o The difference between the hexagonal and the trigonal (in hexagonal setting) is subtle It is hexagonal if the full contents of the unit cell retain the 6 or -6 symmetry shown by the hexagon This is shown by the purple lines in the diagram here But if the contents of the cell reduce the symmetry to a 3-fold axis then it is by definition a axis, trigonal lattice (in the hexagonal setting) o o z x y z x An example of a Trigonal lattice o y A hexagonal lattice can most easily be visualized in the ab plane This reduces the problem to 2 dimensions which is easier to visualize It is called hexagonal because of the six-fold axis described by the faint black lines BUT the hexagon is NOT the unit cell, which is given in red Th unitit cells The ll mustt stack t k together to give the entire lattice Hence the green lozenges represent the multiple unit cells The dashed line is NOT the next unit cell! In this cell, there is “something” at 1/3,2/3,0 This has the effect of lowering the symmetry around the corner lattice point to a 3-fold axis Hence this lattice which otherwise looks “hexagonal” is actually classified as trigonal y z x 2 Lattices and lattice types o o o o o It is useful to consider a crystal structure in terms of a lattice of points An entirely abstract construction; no need for atoms to be located at the lattice points Only certain types of lattices are able to describe real crystals These are described by the different types of unit cells: The smallest repeating unit of a lattice which reflects the full symmetry of the whole lattice Pictures of the basic lattice types o o o Different Lattice Types o - primitive P a cell which has lattice points only at the vertices (and therefore "contains" 8 ×1/8 = 1 lattice point only) - face-centred F a cell which has points in the middle of each face - side-centred A (or B or C) a cell which has points centred on two opposite faces only - body-centred I a cell which has one additional point in the very centre o o o The 14 Bravais lattices Three of these were encountered in Chemistry 2810 to describe the metallic l tti lattices Elemental polonium is thought to be primitive cubic Elemental sodium has a body-centred cubic structure, with a Na atom at each lattice point Elemental magnesium has a face-centred cubic structure with an atom at each lattice point But the lattice types are not just of cubic symmetry (despite the diagrams!) We apply these types to the 7 crystal systems Do not get 7 × 4 = 28 lattices; only 14! Side-centred A (or B or C) Alternate figures of the Bravais lattices This is Fig. 2.8 from “the Massa”! I will try to use these so called “Pearson” labels for the Bravais lattices. 3
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