The crystal lattice and the unit cell are the two cardinal ideas in materials science and crystallography. It is a three-dimensional, repeating structure of points that turn into the atomic, ionic, or molecular positions of atoms in a crystal. Such a structured pattern extends throughout, giving a unique and orderly structure to the material. The unit cell is the smallest building block of the crystal lattice that can be repeated in space to form the entire lattice. The knowledge of these concepts has become very important while analyzing and predicting properties of materials, as the arrangement of atoms within a crystal lattice determines many of their physical and chemical characteristics. It opens up an avenue for scientists and engineers to design and develop materials with predefined properties, thus pushing further quite a large range of technological and industrial applications.
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In the three-dimensional crystal structure, a unit cell is characterized by:
(i) its dimensions along the three edges a, b, and c. These edges may or may not be mutually perpendicular.
(ii) angles between the edges, α (between b and c), β (between a and c), and γ (between a and b). Thus, a unit cell is characterized by six parameters a, b, c, α, β, and γ.
These parameters of a typical unit cell are shown in Fig given below:
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Primitive and Centred Unit Cells
Primitive Unit Cells
When constituent particles are present only on the corner positions of a unit cell, it is called as primitive unit cell.
Centered Unit Cells
When a unit cell contains one or more constituent particles present at positions other than corners in addition to those at corners, it is called a centered unit cell. Centered unit cells are of three types:
Inspection of a wide variety of crystals leads to the conclusion that all can be regarded as conforming to one of the seven regular figures. These basic regular figures are called seven-crystal systems.
Seven Primitive Unit Cells and Their Possible Variations as Centred Unit Cells
Crystal system | Bravias lattices | Intercepts | Interfacial angle | Examples |
Cubic | Primitive, face-centered, body-centered = 3 | a = b = c | ⍺ = β = ? = 90o | Ag, Au, Hg, Pb, diamond, NaCl, ZnS |
Orthorhombic | Primitive, face-centered, body-centered, end centered = 4 | a ≠ b ≠ c | ⍺ = β = ? = 90o | K2SO4,KNO2, BaSO4, Rhombic Sulphur |
Tetragonal | Primitive, body-centred = 2 | a = b ≠ c | ⍺ = β = ? = 90o | TiO2, SnO2, CaSO4, White Tin |
Monoclinic | Primitive, end centered = 2 | a ≠ b ≠ c | ⍺ = ? = 90 β ≠ 90o | CaSO4.2H2O |
Triclinic | Primitive = 1 | a ≠ b ≠ c | ⍺ ≠ β ≠ ? ≠ 90o | CuSO4.5H2O, K2Cr2O7, H3BO3 |
Hexagonal | Primitive = 1 | a = b ≠ c | ⍺ = β = 90o ? = 120o | Zn, Mg, Cd, SiO2, Graphite, ZnO |
Rhombohedral | Primitive = 1 | a = b = c | ⍺ = β = ? ≠ 90o | Bi, As, Sb, CaCO3, HgS |
Total = 14 |
Unit Cells of 14 Types of Bravais Lattices
Any crystal lattice is made up of a very large number of unit cells and every lattice point is occupied by one constituent particle (atom, molecule or ion).
Primitive Cubic Unit Cell
The primitive cubic unit cell has atoms only at its corner. Each atom at a corner is shared between eight adjacent unit cells as shown in Fig. given below:
four unit cells in the same layer and four unit cells in the upper (or lower) layer. Therefore, only 1/8th of an atom (or molecule or ion) actually belongs to a particular unit cell. In Fig. given below, a primitive cubic unit cell has been depicted in three different ways. Each small sphere in this figure represents only the center of the particle occupying that position and not its actual size. Such structures are called open structures.
The arrangement of particles is easier to follow in open structures as shown in the figure given below depicts a space-filling representation of the unit cell with actual particle size
The figure given below shows the actual portions of different atoms present in a cubic unit cell. In all, since each cubic unit cell has 8 atoms on its corners, the total number of atoms in one unit cell 8x(1/8) = 1 atom.
Body Centred Cubic Unit Cell
A body-centred cubic (bcc) unit cell has an atom at each of its corners and also one atom at its body centre. The figure given below depicts (a) open structure (b) space-filling model and (c) the unit cell with portions of atoms actually belonging to it. It can be seen that the atom at the body centre wholly belongs to the unit cell in which it is present.
Thus in a body-centered cubic (bcc) unit cell:
Face Centred Cubic Unit Cell
A face-centered cubic (fcc) unit cell contains atoms at all the corners and at the center of all the faces of the cube. It can be seen in the figure given below, that each atom located at the face-centre is shared between two adjacent unit cells and only ½ of each atom belongs to a unit cell.
The fig. given below depicts (a) an open structure (b) a space-filling model and (c) the unit cell with portions of atoms actually belonging to it.
Thus, in a face-centred cubic (fcc) unit cell:
Also, students can refer,
For a better understanding of the topic and to learn more about crystal Lattices and Unit Cells with video lesson we provide the link to the
YouTube video:
Example 1
Question: The smallest repeating pattern which when repeated in 3-D results in the crystal of substance is called:
1) Space lattice
2) Crystal lattice
3) (correct) Unit cell
4) Bravais lattice
Solution: The unit cell is the smallest repeating unit in the crystal which has all the properties of a crystal. Hence, the answer is the option (3).
Example 2
Question: The most unsymmetrical crystal system is:
1) Cubic
2) Hexagonal
3) (correct) Triclinic
4) Orthorhombic
Solution: The triclinic crystal system has the parameters a neq b neq c and alpha neq beta neq gamma
Example 3
Question: The crystal system of a compound with unit cell dimensions
1) (correct) Hexagonal
2) Cubic
3) Rhombohedral
4) Orthorhombic
Solution: For hexagonal systems, the conditions are a = b neq c and
Example 4
Question: For which of the given crystal families does the following relation hold? a not equal b not equal c and
1) (correct) Monoclinic
2) Triclinic
3) Orthorhombic
4) Hexagonal
Solution: The given relation corresponds to the monoclinic crystal system. Hence, the answer is the option (1).
Example 5
Question: The crystal system characterized by a = b = c and
1) Cubic
2) Tetragonal
3) (correct) Orthorhombic
4) Rhombohedral
Solution: The cubic crystal system has equal edge lengths and all angles equal to
NCERT Chemistry Notes:
Crystal lattices and unit cells form the very essence of crystallography and material science. A crystal lattice is, in essence, a three-dimensional construct of points showing the position of atoms, ions, or molecules of a crystal. It is repeated in a pattern throughout the crystal, thus directly influencing its properties. Unit cells are small units that repeat in these lattices, defining the structure and the overall symmetry of the crystal. The shape and size of the unit cell differ for different types of crystals, and both determine the physical and chemical features that a given material expresses. In order to design materials with specified properties, an understanding of crystal lattices and unit cells is important, also allowing for an analysis of crystal behavior in many applications
The lattice parameters or lattice constant can be defined as the quantities which specify a unit cell. These parameters (constants) are of six types. The dimensions along the edges of a unit cell are represented by a, b and c along x, y and z planes respectively and angle between b and c is represented by α, angle between a and c by β and angle between a and b by γ.
crystal lattice can be of seven types: triclinic, monoclinic, orthorhombic, hexagonal, rhombohedral, tetragonal, and cubic. These collections of crystal lattice are called the Bravais lattices.
It is a type of solid, in which the atoms (or) molecules are not arranged in an orderly manner that is, the same atomic groups are arranged more randomly.
Example: Plastic, rubber
The study of the geometric form and other physical properties of crystalline solids, using x-rays, or electron beam, or neuron beam etc is termed as the science of crystallography.
A crystal in which solid contains only one crystal. These single crystals are produced artificially from their vapor (or) Liquid State.
A crystal structure in which has an aggregate of many small crystals or, grains separated by well-defined grain boundaries. These crystals will have a sharp melting point. Examples: Diamond, Copper, Platinum, Silver, Polonium, Gold, Aluminium, Nickel, Cadmium, Iron etc.
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