PHD → Inorganic chemistry → Solid state chemistry ↓
Crystal structures and lattices
In the fascinating world of solid state chemistry, one of the fundamental concepts is crystal structure. Understanding crystal structures is essential for anyone delving into the chemistry and physics of solids. Crystal structures define the ordered arrangement of atoms, ions, or molecules in a crystalline substance and significantly affect the physical properties of the substance.
Introduction to crystals
A crystal is a solid material whose atoms are arranged in a highly ordered, repetitive pattern spanning all three spatial dimensions. The repeating unit in this ordered structure is known as the unit cell, the smallest part of the crystal lattice that, when repeated, recreates the entire crystal structure.
The study of the formation of crystals and crystal lattices falls under the field of crystallography, which uses a variety of techniques to determine the arrangement of atoms within a solid.
Unit cells and lattices
A unit cell is defined by its lattice parameters, which are the lengths of the edges of the cell and the angles between them. The most straightforward examples of a unit cell are those of the cubic lattice, where the angles between the edges are 90 degrees, and the length of each edge is equal.
Type of mesh | Length of edges | interaxial angle Simple Cube | a = b = c | α = β = γ = 90° Body-centered cubic (BCC) | a = b = c | α = β = γ = 90° Face-centered cubic (fcc) | a = b = c | α = β = γ = 90°
Different materials can crystallize in different lattice systems, which are broadly classified into seven crystal systems:
- Cube - Quadrilateral - Orthorhombic - Hexagonal - Rhomboid - Monoclinic - Triclinic
Seven crystal systems
Each of these crystal systems has its own distinctive features:
- Cubic: Characterized by three perpendicular axes of equal length. Example: Sodium chloride (NaCl).
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- Tetragonal: Similar to a cube but with one axis longer. Example: white tin (Sn).
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- Orthorhombic: All three axes are of different length. Example: Sulfur (S).
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- Hexagonal: Two axes of equal length at 120° and a third axis perpendicular to the plane of the other two. Example: graphite.
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- Rhombus: Also called triangular. All axes are of equal length and all angles are equal but not 90°. Example: Calcite (CaCO3).
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- Monoclinic: Axes of unequal length, with two angles at 90° and one angle just off. Example: gypsum (CaSO4·2H2O).
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- Triclinic: The least symmetrical. All sides and angles are different. Example: Potassium dichromate (K2Cr2O7).
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Close packing in a crystal
In nature, many crystalline structures form through a process called close packing. Close packing involves arranging spheres (representing atoms) in such a way that they occupy the maximum possible space with the least empty volume.
Types of close packing
- Hexagonal close-packed (HCP): This arrangement can be represented as a repeating ABAB pattern. Each atom is surrounded by 12 other atoms. Example: Magnesium (Mg).
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- Face-centered cubic (FCC): This system is also known as cubic close-packed (CCP) and follows the pattern ABCABC. This is the structure of many metals such as aluminum (Al).
Layer A: oooo Layer B: ooo Layer C: oooo
Cubic crystal structures
Many everyday metals and alloys crystallize in cubic structures because of their symmetry and simplicity.
Simple Cube (SC)
In the simple cubic structure, the atoms are located at each corner of the cube. It has a cubic primitive (or net) of one atom per unit cell.
Body-Centered Cubic (BCC)
In the BCC structure, atoms are found at all eight corners as well as one atom at the center of the cube. Iron (Fe) is a classic example of this. This arrangement provides more effective packing than the simple cube.
Face-centered cubic (FCC)
In the FCC structure, atoms are located at each corner and the centre of all the cube faces. This arrangement gives it high packing efficiency and is found in metals such as copper (Cu).
Understanding Coordination Number and Atomic Packing Factor
The coordination number is the number of nearest neighbors surrounding an atom in a crystal structure. The atomic packing factor (APF) is the fraction of the volume in a crystal structure that is occupied by atoms.
Cubic structures and their properties
Below are the properties of simple, body-centered and face-centered cubic structures:
Structure type | Coordination number | Atomic packing factor Simple cube | 6 | 0.52 Body-Centered Cubic (BCC) | 8 | 0.68 Face-Centered Cubic (FCC) | 12 | 0.74
Illustration of crystal structures
Consider a simple cubic structure represented visually in a grid, where there is an atom at each corner of the cube:
, , , , ,
In short, the study of crystal structures and lattices provides deep insights into the physical properties of materials, affecting everything from electrical conductivity to mechanical strength. The orderly arrangement of atoms, the regularity of lattice structures, and the beauty of crystallographic systems play a key role in defining the characteristics of the materials we encounter in both nature and industry.
Conclusion
Exploring crystal structures and lattices is crucial in understanding the chemical and physical behaviour of materials. From simple cubes to complex polygons, each arrangement reveals the complexities and beauty of solid matter. As we delve deeper into solid state chemistry, these fundamental concepts pave the way towards innovation and discovery in materials science.