Elasticity deals with the behaviour of solids when external forces cause deformation and how the body regains its original shape after the forces are removed.
1. Intermolecular / Interatomic Forces
- In a solid at equilibrium, atoms or molecules are separated by an equilibrium distance r₀.
- At r₀, the force between atoms is zero and potential energy is minimum.
- If distance < r₀ → repulsive force acts.
- If distance > r₀ → attractive force acts.
- Atoms in solids behave like they are connected by stiff springs.
2. Elasticity
- Elasticity is the property of a material by which it regains its original shape and size after removal of deforming forces.
- Deforming force: External force causing change in shape or size.
- Restoring force: Internal force opposing deformation.
- If a body does not regain original shape, it is called plastic.
3. Stress
Stress is the restoring force per unit area.
Stress = F / A
- Normal stress → force perpendicular to area
- Tangential stress → force parallel to area
- Stress is a scalar quantity
Unit: N m−2 (Pascal)
4. Strain
Strain is the fractional change in dimension.
Strain = Change in dimension / Original dimension
- Strain has no unit and is dimensionless
- It is a scalar quantity
Types of Strain
- Longitudinal Strain: ΔL / L
- Volumetric Strain: ΔV / V
- Shearing Strain: tan θ ≈ θ
5. Hooke’s Law
Within elastic limit:
Stress ∝ Strain
Stress = E × Strain
- The range where Hooke’s law is valid is called the proportional limit.
- Beyond elastic limit, permanent deformation occurs.
6. Moduli of Elasticity
(a) Young’s Modulus (Y)
Y = (F / A) / (ΔL / L)
Measures resistance to change in length.
(b) Bulk Modulus (B)
B = −ΔP / (ΔV / V)
Measures resistance to change in volume.
(c) Modulus of Rigidity (η)
η = Tangential stress / Shearing strain
Measures resistance to change in shape.
7. Poisson’s Ratio (σ)
σ = Lateral strain / Longitudinal strain
- Value lies between 0.1 and 0.3 for most materials
- Negative sign indicates decrease in radius on stretching
Relation between elastic constants:
Y = 3B(1 − 2σ) = 2η(1 + σ)
8. Elastic Hysteresis
- Difference in loading and unloading stress–strain curves
- Area of loop represents energy lost
- Materials with high hysteresis are used as vibration absorbers
9. Elastic Potential Energy
Energy stored in a stretched wire:
U = ½ × stress × strain × volume
U = ½ Y × strain² × volume
Energy density:
u = U / V = ½ Y × strain²
10. Important Applications
- Change in density with pressure: ρ = ρ₀ (1 + CP)
- Angle of twist: Lφ = rθ
- Twisting couple: C = πηr⁴ / 2L
- Bending of beam (rectangular): δ = MgL³ / 4bd³Y
- Bending of beam (circular): δ = MgL³ / 12πr⁴Y
Last modified: December 14, 2025
