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SOLID STATE Crystals Crystal structure basics unit cells symmetry

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Presentation on theme: "SOLID STATE Crystals Crystal structure basics unit cells symmetry"— Presentation transcript:

1 SOLID STATE Crystals Crystal structure basics unit cells symmetry
lattices Diffraction how and why - derivation Some important crystal structures and properties close packed structures octahedral and tetrahedral holes basic structures ferroelectricity

2 Objectives By the end of this section you should:
be able to identify a unit cell in a symmetrical pattern know that there are 7 possible unit cell shapes be able to define cubic, tetragonal, orthorhombic and hexagonal unit cell shapes

3 Why study crystal structures?
Why Solids?  most elements solid at room temperature  atoms in ~fixed position “simple” case - crystalline solid  Crystal Structure Why study crystal structures?  description of solid  comparison with other similar materials - classification  correlation with physical properties

4 Crystals are everywhere!

5 More crystals

6 Early ideas Crystals are solid - but solids are not necessarily crystalline Crystals have symmetry (Kepler) and long range order Spheres and small shapes can be packed to produces regular shapes (Hooke, Hauy) ?

7 Group discussion Kepler wondered why snowflakes have 6 corners, never 5 or 7. By considering the packing of polygons in 2 dimensions, demonstrate why pentagons and heptagons shouldn’t occur.

8 Definitions 1. The unit cell
“The smallest repeat unit of a crystal structure, in 3D, which shows the full symmetry of the structure” The unit cell is a box with: 3 sides - a, b, c 3 angles - , , 

9  Seven unit cell shapes
Cubic a=b=c ===90° Tetragonal a=bc ===90° Orthorhombic abc ===90° Monoclinic abc ==90°,   90° Triclinic abc     90° Hexagonal a=bc ==90°, =120° Rhombohedral a=b=c ==90° Think about the shapes that these define - look at the models provided.

10 2D example - rocksalt (sodium chloride, NaCl)
We define lattice points ; these are points with identical environments

11 Choice of origin is arbitrary - lattice points need not be atoms - but unit cell size should always be the same.

12 This is also a unit cell - it doesn’t matter if you start from Na or Cl

13 - or if you don’t start from an atom

14 This is NOT a unit cell even though they are all the same - empty space is not allowed!

15 In 2D, this IS a unit cell In 3D, it is NOT

16 All M. C. Escher works (c) Cordon Art-Baarn-the Netherlands
All M.C. Escher works (c) Cordon Art-Baarn-the Netherlands. All rights reserved.

17 Examples The sheets at the end of handout 1 show examples of periodic patterns. On each, mark on a unit cell. [remembering that there are a number of different (correct) answers!]

18 Summary All unit cells must be identical
Unit cells must link up - cannot have gaps between adjacent cells All unit cells must be identical Unit cells must show the full symmetry of the structure  next section


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