Young’s Modulus ($E$): Ratio of stress to strain in the linear elastic region, $\displaystyle E = \frac{\sigma}{\epsilon}$.
Units and Dimensions
Quantity
SI Unit
Symbol
Force
newton (N)
F
Area
square metre (m²)
A
Stress
pascal (Pa) = N·m⁻²
σ
Length
metre (m)
L
Strain
dimensionless
ε
Young’s Modulus
pascal (Pa)
E
Stress–Strain Relationship
For most engineering materials the initial portion of the stress‑strain curve is linear. In this region:
$$\sigma = E \, \epsilon$$
Beyond the proportional limit the material yields and the relationship becomes non‑linear.
Example Calculation
Given: A steel rod of original length $L_0 = 2.00\ \text{m}$ and cross‑sectional area $A = 5.0 \times 10^{-4}\ \text{m}^2$ is subjected to a tensile force $F = 10\,000\ \text{N}$.
Stress is not the same as pressure; stress acts on a specific plane within a material.
Strain is dimensionless; it is not measured in metres.
Young’s modulus is a material property; it does not depend on the dimensions of the sample.
Suggested diagram: Typical stress‑strain curve showing the elastic region, proportional limit, yield point, and fracture.
Practice Questions
Calculate the stress in a copper wire of diameter $2.0\ \text{mm}$ carrying a force of $500\ \text{N}$.
A polymer has $E = 1.5 \times 10^{9}\ \text{Pa}$. If a tensile load produces a stress of $3.0 \times 10^{6}\ \text{Pa}$, what is the resulting strain?
Explain why the stress‑strain curve for brittle materials differs from that of ductile materials.
Summary
Stress, strain and Young’s modulus provide a quantitative framework for describing how materials respond to external forces. Mastery of these concepts enables accurate prediction of deformation and failure in engineering applications.