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.