1. Elasticity and Plasticity

Elasticity: The property of a body by virtue of which it tends to regain its original shape and size after the deforming force is removed.

Plasticity: The property by which a body does not regain its original shape/size after the deforming force is removed — the deformation is permanent.

  • Perfectly elastic body: Regains original shape completely — ideal, no real body is perfectly elastic. Quartz fibre comes closest.
  • Perfectly plastic body: Retains deformed shape completely — putty, clay.
  • Real materials lie between these extremes — steel is highly elastic; lead is highly plastic.

Elastic limit: The maximum stress up to which a body shows elastic behaviour. Beyond this, permanent deformation sets in.

2. Stress

When a deforming force F is applied to a body, an internal restoring force develops. Stress is defined as the restoring force per unit area of cross-section:

Stress=FA
SI unit: N m2=Pa (pascal)

Types of Stress

TypeDirection of force relative to areaEffect
Tensile stressPerpendicular (outward) — stretchingElongation
Compressive stressPerpendicular (inward) — compressionShortening
Shear (tangential) stressParallel to the surface — tangentialChange in shape (no volume change)
Hydraulic (bulk) stressNormal from all sides — uniform pressureChange in volume (no shape change)

Tensile and compressive stresses are together called longitudinal stress or normal stress.

3. Strain

Strain is the ratio of the change in configuration to the original configuration. It is dimensionless — no units.

TypeFormulaCaused by
Longitudinal (linear) strainε=ΔLL0Tensile or compressive stress
Shear strainϕ=xL=tanϕϕ (for small angles)Tangential (shear) stress
Volumetric (bulk) strain=ΔVV0Hydraulic (uniform) stress

Worked Example

A wire of length 2 m extends by 0.5 mm when loaded. Longitudinal strain:

ε=ΔLL0=0.5×1032.0=2.5×104

4. Hooke's Law

StressStrain
Stress=E×Strain

where E is the modulus of elasticity (a material constant with units of Pa).

  • Valid only within the proportionality limit — below the elastic limit.
  • The proportionality constant E depends on the material, not on the dimensions of the body.
  • Higher E → stiffer material (less strain for same stress).

5. Stress-Strain Curve

When a wire is gradually loaded, the stress-strain graph passes through several distinct regions:

Point/RegionNameBehaviour
O → AProportionality limit (A)Linear; stress ∝ strain exactly; Hooke's law strictly obeyed
A → BElastic limit (B)Non-linear but still elastic; body returns to original shape if force removed; Hooke's law no longer exact
B → CYield point (C) / Upper yield pointBeyond elastic limit; permanent deformation begins; strain increases without much increase in stress
C → DPlastic regionPlastic flow (necking begins); material elongates significantly with little increase in load
DUltimate tensile stress (UTS)Maximum stress the material can withstand; cross-sectional area decreases (necking)
EFracture point / Breaking pointWire breaks; stress at fracture < UTS (due to necking)

Ductile vs Brittle Materials

PropertyDuctile (e.g., steel, copper)Brittle (e.g., glass, cast iron)
Plastic regionLarge — significant plastic deformation before fractureVery small — fractures very soon after elastic limit
UTS vs fracture stressClear gap — necking visibleFracture ≈ UTS (almost coincide)
Warning before fractureVisible (elongation)None — sudden failure
Area under stress-strainLarge (absorbs more energy)Small

Elastomers (Rubber-like materials)

Elastomers (e.g., rubber, tissue) show large strains for small stresses — they do not obey Hooke's law over a wide range. The stress-strain curve is nonlinear and shows hysteresis. The elastic limit is very high, and no well-defined plastic region exists.

6. Worked Example — Stress on a Wire

A steel wire of diameter 2 mm supports a load of 10 N. Find the stress.

r=1 mm=103 m

A=πr2=π×(103)2=3.14×106 m2

Stress=FA=103.14×106=3.18×106 Pa