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The Young modulusAQA A-Level Physics: Revision notes

Section 1

Tensile stress and strain

A material under tension is described using two quantities that do not depend on the size of the sample.

Tensile stress is the force per unit cross-sectional area: σ=FA\sigma = \frac{F}{A}, measured in pascals (Pa, or N m⁻²).

Tensile strain is the extension per unit original length: ε=ΔLL\varepsilon = \frac{\Delta L}{L}. It is a ratio, so it has no unit.

For a wire of diameter dd, the area is A=πd24A = \frac{\pi d^2}{4}. Convert mm to m before calculating.

Key termstensile stresstensile strain
Common mistake

Using the diameter as the radius, or leaving the diameter in mm. A wire of diameter 0.80 mm has radius 0.40 × 10⁻³ m.

Section 2

The Young modulus

Within the limit of proportionality, stress is proportional to strain. The constant of proportionality is the Young modulus:

E=tensile stresstensile strain=FLAΔLE = \frac{\text{tensile stress}}{\text{tensile strain}} = \frac{F L}{A \Delta L}

It is measured in pascals (Pa). A material with a high Young modulus, such as steel, is stiff: it needs a large stress to produce a given strain. Because stress and strain remove the effect of size, the Young modulus is a property of the material and not of a particular sample.

Key termsYoung modulusstiff
Exam tip

For two samples of the same material, extension is proportional to force and length, and inversely proportional to area. Doubling the diameter divides the extension by 4.

Section 3

Worked example

A copper wire of length 2.0 m and diameter 0.50 mm carries a tension of 30 N. E=1.2×1011E = 1.2 \times 10^{11} Pa.

Area: A=π×(0.25×10−3)2=1.96×10−7A = \pi \times (0.25 \times 10^{-3})^2 = 1.96 \times 10^{-7} m²

Stress: σ=30/1.96×10−7=1.53×108\sigma = 30 / 1.96 \times 10^{-7} = 1.53 \times 10^{8} Pa

Strain: ε=1.53×108/1.2×1011=1.27×10−3\varepsilon = 1.53 \times 10^{8} / 1.2 \times 10^{11} = 1.27 \times 10^{-3}

Extension: ΔL=1.27×10−3×2.0=2.5×10−3\Delta L = 1.27 \times 10^{-3} \times 2.0 = 2.5 \times 10^{-3} m

Section 4

Stress–strain graphs

A graph of stress (vertical axis) against strain (horizontal axis) for a metal is a straight line through the origin at low stress. Its gradient is the Young modulus.

To find EE from a graph, draw a large triangle on the straight section and calculate change in stress ÷ change in strain. Do not use points beyond the straight line, because stress is no longer proportional to strain there. A steeper line means a larger Young modulus, so a stiffer material.

If the graph is plotted as force against extension, the gradient is F/ΔLF / \Delta L, so E=gradient×LAE = \text{gradient} \times \frac{L}{A}.

Key termsgradient
Common mistake

Using a single point to find E. Use the gradient of the line of best fit, which reduces the effect of random errors.

Section 5

Required practical 4: Young modulus of a wire

Method: clamp a long thin wire (about 2 m) at one end and pass it over a pulley, adding masses to a hanger at the other end. Use a fiducial marker on the wire and a metre rule to measure its extension.

  1. Measure the unstretched length LL from the clamp to the marker with a metre rule
  2. Measure the diameter with a micrometer at several points along the wire and in two perpendicular directions, then take the mean
  3. Add masses in equal steps, recording the extension each time, and also record while unloading
  4. Plot force against extension, find the gradient, and calculate E=gradient×L/AE = \text{gradient} \times L / A

Errors: the diameter is the largest source of percentage uncertainty because it is small and is squared. Use a long wire to make the extension large, and keep the loads small enough to stay within the limit of proportionality. Wear safety goggles in case the wire snaps, and place a box of sand or cloth below to catch the masses.

Key termsmicrometerlimit of proportionality
Exam tip

Say why a long, thin wire is used: it gives a larger extension that can be measured with smaller percentage uncertainty.

Must Know

  • Stress = F / A, in Pa; strain = ΔL / L, with no unit
  • E=stress/strain=FL/(AΔL)E = \text{stress} / \text{strain} = F L / (A \Delta L)
  • The Young modulus is a property of the material, measured in Pa
  • On a stress–strain graph, the gradient of the straight section is E
  • Measure the diameter with a micrometer at several points and use the mean
  • Diameter is the main uncertainty because the area depends on d²

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Exam questions on The Young modulus

  1. A steel wire of length 2.50 m and diameter 0.80 mm hangs from a fixed support and carries a load that produces a tension of 40 N. The Young modulus of the steel is 2.0 × 10¹¹ Pa and the wire obeys Hooke's law.
    Calculate the extension of the wire.2 marks
  2. Two rods, X and Y, have identical lengths of 1.50 m and identical cross-sectional areas of 2.0 × 10⁻⁵ m². The Young modulus of X is 1.0 × 10¹¹ Pa and the Young modulus of Y is 2.0 × 10¹¹ Pa. Both rods are used within the limit of proportionality.
    Calculate the force needed to produce an extension of 0.80 mm in rod X.2 marks
  3. A student determines the Young modulus of a copper wire. The wire is fixed at one end and passes over a pulley at the other end, where masses are added in steps. The unstretched length from the fixed end to a marker is 1.85 m. The student measures the diameter of the wire with a micrometer and obtains a mean value of 0.30 mm. A graph of force against extension is a straight line through the origin with a gradient of 4.5 × 10³ N m⁻¹.
    Explain how the student should measure the diameter of the wire, and why this measurement is likely to be the largest source of uncertainty in the Young modulus.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).