Crystallography | Anna University engineering physics notes

CRYSTALLOGRAPHY

Introduction
Matter exists around us in different forms, but solids are among the most structurally fascinating states of matter. 
From smartphone screens to diamonds in jewelry, solids play an important role in modern technology and engineering. 

The study of solids forms the foundation of:
  • Crystallography
  • Solid-State Physics
  • Materials Science
  • Nanotechnology
  • Semiconductor Engineering
 In this article, we explore:
  • The basic nature of solids
  • Physical properties of solids
  • Classification of solids
  • Crystalline materials
  • Amorphous materials
  • Differences between crystalline and amorphous solids
What is a solid?
  1. A solid is a state of matter that possesses a definite shape and definite volume. 
  2. Unlike liquids and gases, particles in a solid cannot move freely from one place to another. Instead, they vibrate about fixed equilibrium positions. This restricted movement gives solids their rigidity and stability.
  3. In solids, atoms, molecules, or ions are closely packed and held together by strong intermolecular or interatomic forces.
Characteristics of solids

1. Definite Shape

Solids retain their shape unless an external force changes it. A metal rod, a wooden block, or a crystal maintains its structure because the particles are fixed in position.


2. Definite Volume

The volume of a solid remains constant under normal conditions because particles are tightly packed and resist compression.


3. Strong Intermolecular Forces

The attractive forces between particles are very strong in solids. These forces hold the particles together and prevent free movement.


4. High Density

Since particles are packed closely, solids generally have higher densities compared to liquids and gases.


5. Negligible Compressibility

Solids cannot be compressed easily because there is very little empty space between particles.


6. Very Slow Diffusion

Diffusion in solids occurs extremely slowly due to restricted particle motion.


At the microscopic level, solids consist of atoms, molecules, or ions arranged in a particular pattern. The arrangement of these particles determines the physical properties of the solid.

Based on particle arrangement, solids are broadly classified into:

  1. Crystalline solids
  2.  Amorphous solids
Types of solids
Crystalline solids

Crystalline solids are solids in which constituent particles are arranged in a highly ordered repeating three-dimensional pattern.

This regular arrangement is known as a crystal lattice.

Examples of crystalline solids include:

  • Diamond
  • Quartz
  • Sodium chloride
  • Ice
  • Copper

Properties of Crystalline Solids

1. Long-Range Order

Particles are arranged periodically over large distances, resulting in a regular structure.


2. Sharp Melting Point

Crystalline solids melt at a fixed temperature. For example, pure ice melts sharply at 0°C under standard atmospheric pressure.


3. Anisotropy

Their physical properties vary with direction. Properties such as electrical conductivity, thermal conductivity, and refractive index may differ along different crystal directions.


4. Definite Geometrical Shape

Crystals possess well-defined faces, edges, and angles due to their ordered arrangement.


5. Cleavage Property

They break along specific planes known as cleavage planes.


Examples of Crystalline Materials

Crystalline solids are extremely important in electronics, metallurgy, semiconductor devices, and optical technologies.



Amorphous solids

Amorphous solids are solids in which particles are arranged randomly without long-range periodic order.

Unlike crystalline materials, amorphous solids do not possess a regular repeating structure.

Common examples include:

  • Glass
  • Rubber
  • Plastics
  • Gel
  • Pitch

Properties of Amorphous Solids

1. Short-Range Order

The arrangement of particles is regular only over very small distances.


2. No Sharp Melting Point

Amorphous solids soften gradually over a range of temperatures rather than melting sharply.


3. Isotropy

Their physical properties are identical in all directions.


4. Irregular Shape

They do not possess geometrically regular structures like crystals.


5. Irregular Fracture

Amorphous solids break into irregular pieces rather than along definite planes.


Examples of Amorphous Materials

Glass is one of the most commonly encountered amorphous solids. Although rigid like a solid, its atomic arrangement resembles that of a liquid.

 Classification of solids based on bonding

Solids can also be classified according to the type of bonding between constituent particles.


1. Ionic Solids

Formed by electrostatic attraction between positive and negative ions.

Examples

  • Sodium chloride (NaCl)
  • Potassium bromide (KBr)

Properties

  • High melting point
  • Hard and brittle
  • Conduct electricity in molten state

2. Covalent Solids

Atoms are connected through covalent bonds.

Examples

  • Diamond
  • Silicon carbide

Properties

  • Extremely hard
  • Very high melting point
  • Usually poor conductors

3. Metallic Solids

Positive metal ions are surrounded by a sea of free electrons.

Examples

  • Copper
  • Iron
  • Silver

Properties

  • Good electrical conductivity
  • Malleable and ductile
  • Lustrous appearance

4. Molecular Solids

Molecules are held together by weak intermolecular forces.

Examples

  • Ice
  • Dry ice
  • Solid carbon dioxide

Properties

  • Soft
  • Low melting point
  • Poor conductors

 Difference Between Crystalline and Amorphous Solids

Property

Crystalline Solids

Amorphous Solids

Particle Arrangement

Ordered and periodic

Random

Melting Point

Sharp

Gradual

Nature

Anisotropic

Isotropic

Structure

Regular

Irregular

Cleavage

Definite planes

Irregular fracture

Order

Long-range

Short-range



Simple Cubic
SPEED
ZOOM

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Simple Cubic (SC) Structure – Derivation

The Simple Cubic (SC) structure is the most basic crystal structure in solid state physics. In this arrangement, atoms are present only at the eight corners of the cube.

Example of Simple Cubic Crystal

  • Polonium (Po)

Number of Atoms per Unit Cell

In Simple Cubic structure, atoms are present only at the corners.

Contribution from one corner atom = 1/8
Total corner contribution = 8 × 1/8 = 1
Total atoms in SC = 1

Atomic Radius Relation

In Simple Cubic structure, atoms touch each other along the cube edge.

Edge length = 2r
a = 2r
r = a/2

Coordination Number

Each atom touches 6 nearest neighboring atoms.

Coordination Number = 6

Atomic Packing Factor (APF)

APF = Volume occupied by atoms / Volume of unit cell
Volume occupied by atoms = (4/3)Ï€r³
Unit cell volume = a³
Using a = 2r
APF = π/6
APF ≈ 0.52
Packing Efficiency = 52%

Important Results

Property Value
Atoms per unit cell 1
Coordination Number 6
Radius Relation a = 2r
Atomic Packing Factor 0.52
Packing Efficiency 52%

Quick Facts

Simple Cubic → Edge Contact

a = 2r

Body-Centered Cubic (BCC) Structure – Derivation

The Body-Centered Cubic (BCC) structure is an important crystal structure in solid state physics. In this structure, atoms are present at the corners and one atom is located at the center of the cube.

Examples of BCC Metals

  • Iron (α-Fe)
  • Chromium
  • Tungsten

Number of Atoms per Unit Cell

Each corner atom is shared by 8 unit cells.

Contribution from one corner atom = 1/8
Total corner contribution = 8 × 1/8 = 1

The body-centered atom belongs completely to the unit cell.

Contribution from body-centered atom = 1
Total atoms in BCC = 1 + 1 = 2

Derivation of Atomic Radius Relation

In BCC, atoms touch each other along the body diagonal.

Body diagonal of cube = √3 a

Along the body diagonal:

r + 2r + r = 4r
√3 a = 4r
r = (√3 a)/4
a = 4r/√3

Coordination Number

The center atom touches 8 nearest neighboring atoms.

Coordination Number = 8

Atomic Packing Factor (APF)

APF = Volume occupied by atoms / Volume of unit cell
Volume occupied by atoms = 2 × (4/3)Ï€r³
Unit cell volume = a³
APF ≈ 0.68
Packing Efficiency = 68%

Important Results

Property Value
Atoms per unit cell 2
Coordination Number 8
Radius Relation √3 a = 4r
Packing Efficiency 68%

Quick Points

BCC → Body Diagonal Contact

√3 a = 4r

Hexagonal Close Packed (HCP) Structure – Derivation

The Hexagonal Close Packed (HCP) structure is one of the most densely packed crystal structures. In HCP arrangement, atoms are packed very closely to achieve maximum packing efficiency.

Examples of HCP Metals

  • Magnesium (Mg)
  • Zinc (Zn)
  • Titanium (Ti)
  • Cadmium (Cd)

Number of Atoms per Unit Cell

In HCP structure:

Corner atoms contribution = 12 × 1/6 = 2
Face-centered atoms contribution = 2 × 1/2 = 1
Middle layer atoms contribution = 3
Total atoms in HCP = 2 + 1 + 3 = 6

Coordination Number

Each atom in HCP touches 12 nearest neighboring atoms.

Coordination Number = 12

Atomic Radius Relation

In HCP structure, atoms touch each other along the hexagonal edge.

Edge length of hexagon = 2r
a = 2r

Ideal c/a Ratio

The ideal height-to-base ratio for HCP structure is:

c/a = 1.633

Therefore,

c = 1.633 a

Atomic Packing Factor (APF)

APF = Volume occupied by atoms / Volume of unit cell
APF ≈ 0.74
Packing Efficiency = 74%

Important Results

Property Value
Atoms per unit cell 6
Coordination Number 12
Radius Relation a = 2r
Ideal c/a Ratio 1.633
Packing Efficiency 74%

HCP and FCC have the highest packing efficiency.

APF = 0.74

To understand crystal planes clearly, read our detailed guide on Miller Indices .

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