understand and use the terms load, extension, compression and limit of proportionality

Stress, Strain and the Limit of Proportionality

Learning Objectives

  • Define load (force), extension, compression and the limit of proportionality (LoP).
  • Distinguish between tensile and compressive loading.
  • Apply Hooke’s law to calculate stress, strain, extension and the spring constant for a rod.
  • Read and interpret a stress–strain graph: locate the linear (elastic) region, LoP, elastic limit, yield point, ultimate tensile strength and fracture.
  • Explain how Young’s modulus relates to the slope of the linear region and to material stiffness.
  • Identify key experimental considerations (area measurement, safety limits, avoiding permanent deformation).

Key Definitions

TermDefinitionTypical Units
Load (Force) $F$ External force applied to a body. Can be tensile (pulling) or compressive (pushing). newton (N)
Extension $\Delta L$ Increase in length under a tensile load: $\Delta L = L - L_{0}>0$. metre (m) or millimetre (mm)
Compression $\Delta L$ Decrease in length under a compressive load: $\Delta L = L - L_{0}<0$. metre (m) or millimetre (mm)
Stress $\sigma$ Force per unit original cross‑sectional area. pascal (Pa) = N m⁻²
Strain $\varepsilon$ Relative change in length; dimensionless (often expressed as a %). dimensionless (or %)
Limit of Proportionality (LoP) Maximum stress at which stress is directly proportional to strain – the end of the straight‑line part of the curve. It is a material‑specific property and **not** the same as the yield point. Pa (stress) or dimensionless (strain)
Elastic Limit Largest stress that can be applied without any permanent (plastic) deformation. For many engineering metals the elastic limit coincides closely with the LoP. Pa
Yield Point Stress at which noticeable plastic deformation begins. May occur at a higher stress than the LoP for ductile materials. Pa
Young’s Modulus $E$ Material constant defined by
$\sigma = E\,\varepsilon$. It is the slope of the linear (elastic) region of a stress–strain graph.
Pa (commonly GPa for metals)

Fundamental Formulas

  • Stress: $\displaystyle \sigma = \frac{F}{A}$ (where $A$ is the original cross‑sectional area).
  • Strain: $\displaystyle \varepsilon = \frac{\Delta L}{L_{0}}$.
  • Hooke’s law (elastic region): $\displaystyle \sigma = E\,\varepsilon$.
  • Spring‑constant form for a straight rod (derived from Hooke’s law):
    $\displaystyle F = k\,\Delta L\qquad\text{with}\qquad k = \frac{EA}{L_{0}}$.

Derivation of $k = EA/L_{0}$

  1. Start with $\sigma = E\varepsilon$.
  2. Replace $\sigma$ by $F/A$ and $\varepsilon$ by $\Delta L/L_{0}$:
    $\displaystyle \frac{F}{A}=E\frac{\Delta L}{L_{0}}$.
  3. Re‑arrange to obtain $F = \left(\frac{EA}{L_{0}}\right)\Delta L$; the term in brackets is the spring constant $k$ for the rod.

Typical Values of Young’s Modulus

MaterialYoung’s Modulus $E$ (GPa)
Structural steel≈ 200 – 210
Aluminium≈ 69
Copper≈ 110
Concrete (compressed)≈ 30 – 40
Polymers (e.g., PMMA)≈ 3 – 5

Stress–Strain Graph (Cambridge A‑Level)

Typical stress–strain curve showing linear region, LoP, elastic limit, yield point, ultimate tensile strength and fracture
Key points on the curve (coloured arrows in the diagram):
  1. Linear (elastic) region – slope = $E$.
  2. Limit of Proportionality (LoP) – end of straight‑line behaviour.
  3. Elastic limit – maximum stress with fully recoverable deformation (often coincides with LoP for metals).
  4. Yield point – start of noticeable plastic deformation.
  5. Ultimate tensile strength (UTS) – highest stress attained.
  6. Fracture – material breaks.

Graph‑Reading Exercise

  1. Estimate the stress at the LoP ($\sigma_{\text{LoP}}$) from the vertical axis.
  2. Using the data in the example below, calculate the stress produced by the given load. Compare it with $\sigma_{\text{LoP}}$ and state whether the load lies within the linear region.
  3. Read the strain at the yield point. Comment on the difference between the LoP and the yield point for a ductile metal such as steel.

Worked Example – Elastic Extension of a Steel Rod

Given:

  • Original length $L_{0}=1.20\ \text{m}$
  • Diameter $d=1.80\ \text{cm}$ → $A=\dfrac{\pi d^{2}}{4}=2.54\times10^{-4}\ \text{m}^{2}$
  • Young’s modulus $E=2.0\times10^{11}\ \text{Pa}$
  • Tensile load $F=5.0\times10^{4}\ \text{N}$ (assumed to be within the elastic region)
  1. Stress: $\displaystyle \sigma=\frac{F}{A}= \frac{5.0\times10^{4}}{2.54\times10^{-4}}=1.97\times10^{8}\ \text{Pa}$.
  2. Strain (Hooke’s law): $\displaystyle \varepsilon=\frac{\sigma}{E}= \frac{1.97\times10^{8}}{2.0\times10^{11}}=9.85\times10^{-4}$ (≈ 0.098 %).
  3. Extension: $\displaystyle \Delta L = \varepsilon L_{0}= (9.85\times10^{-4})(1.20)=1.18\times10^{-3}\ \text{m}=1.18\ \text{mm}$.
  4. From the typical steel curve, $\sigma_{\text{LoP}}\approx2.0\times10^{8}\ \text{Pa}$. Since $\sigma=1.97\times10^{8}\ \text{Pa}<\sigma_{\text{LoP}}$, the load is safely within the linear region.

Distinguishing Tensile and Compressive Loading

  • Tensile loading: pulls the material, giving a positive extension ($\Delta L>0$) and a positive stress ($\sigma>0$).
  • Compressive loading: pushes the material, giving a negative extension ($\Delta L<0$) and a negative stress ($\sigma<0$). In practice the magnitude of compressive stress is quoted as a positive number, but the loading type must be noted.
  • Both obey $\sigma = E\varepsilon$ while the material remains in the elastic region.

Common Misconceptions – Clarified

  • Load vs. Stress: Load is the total force $F$ (N). Stress is the force per unit area ($\sigma = F/A$) and has units of pressure (Pa).
  • Extension vs. Strain: Extension $\Delta L$ is an absolute change in length (m). Strain $\varepsilon$ is the relative change ($\Delta L/L_{0}$) and is dimensionless.
  • LoP vs. Yield Point: LoP marks the end of the proportional (linear) relationship. The yield point marks the onset of permanent deformation; they may be close for many metals but are distinct concepts.
  • Units: Stress → Pa (or N mm⁻²). Strain → dimensionless (often expressed as a %). They are not interchangeable.

Typical Linear‑Elastic Strain Ranges

  • Steel: up to ≈ 0.20 % strain ($2\times10^{-3}$) before noticeable deviation.
  • Aluminium: up to ≈ 0.15 % strain.
  • Copper: up to ≈ 0.25 % strain.
  • Polymers (e.g., PMMA): up to 1 %–2 % strain.

Experimental & Safety Considerations

  • Measure the cross‑sectional area accurately (calipers for diameter, then $A=\pi d^{2}/4$ for circular rods; $A=wh$ for rectangular bars).
  • Apply loads gradually; record extension after each increment to avoid sudden fracture.
  • Never exceed the ultimate tensile strength shown on the stress–strain curve – failure is catastrophic.
  • When using a universal testing machine, set the maximum load just below the estimated $\sigma_{\text{LoP}}$ for a first trial.
  • Always wear safety goggles and keep a safe distance from the testing apparatus.

Symbol Summary

SymbolNameUnitExpression
$F$Load (Force)NGiven or measured
$A$Cross‑sectional areaMeasured directly or calculated
$\sigma$StressPa$\sigma = \dfrac{F}{A}$
$\Delta L$Extension (tension) or compressionm$\Delta L = L - L_{0}$
$\varepsilon$Straindimensionless (or %)$\varepsilon = \dfrac{\Delta L}{L_{0}}$
$E$Young’s modulusPa (often GPa)$E = \dfrac{\sigma}{\varepsilon}$
$k$Spring constant of a rodN m⁻¹$k = \dfrac{EA}{L_{0}}$
LoPLimit of ProportionalityPa (stress) or dimensionless (strain)Maximum stress where $\sigma \propto \varepsilon$
Elastic limitMaximum stress with fully recoverable deformationPa≈ LoP for many metals
Yield pointOnset of permanent (plastic) deformationPaUsually slightly above LoP for ductile materials

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