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This lesson brings together all the concepts from the materials topic into multi-step problems, experimental design questions, and material selection challenges. These are the types of questions that appear frequently in Edexcel A-level Physics papers and require you to combine several equations and concepts.
Before tackling problems, here is a reference of all the equations used in this topic:
| Equation | Variables | When to use |
|---|---|---|
| ρ = m/V | Density, mass, volume | Density calculations |
| p = ρgh | Pressure, density, depth | Fluid pressure at depth |
| F = kx | Force, spring constant, extension | Hooke’s law (within limit of proportionality) |
| E = ½kx² = ½Fx | Elastic PE, spring constant, extension | Energy stored in a spring |
| σ = F/A | Stress, force, area | Stress in a material |
| ε = ΔL/L | Strain, extension, original length | Strain in a material |
| E = σ/ε = FL/(AΔL) | Young modulus, stress, strain | Stiffness of a material |
| F_upthrust = ρVg | Upthrust, fluid density, volume | Archimedes’ principle |
| A = πd²/4 | Area, diameter | Cross-sectional area of a wire |
Problem 1: A cylindrical storage tank is filled with oil of density 850 kg m⁻³ to a depth of 6.0 m. The tank has a flat circular base of diameter 3.0 m. Calculate (a) the pressure at the base due to the oil, and (b) the force exerted on the base by the oil.
(a) Pressure = ρgh = 850 × 9.81 × 6.0 = 50 031 Pa ≈ 50.0 kPa
(b) Area of base = πr² = π × (1.5)² = 7.069 m² Force = pressure × area = 50 031 × 7.069 = 353 700 N ≈ 354 kN
Note: This is the force due to the oil only. The total force on the base also includes the force from atmospheric pressure above the oil.
Problem 2: A spring of spring constant 400 N m⁻¹ is compressed by 0.12 m and used to launch a 0.050 kg ball vertically upward. Assuming all the elastic potential energy is converted to gravitational potential energy, calculate the maximum height reached by the ball.
Energy stored = ½kx² = ½ × 400 × (0.12)² = 2.88 J
At maximum height: mgh = 2.88 h = 2.88 / (0.050 × 9.81) = 2.88 / 0.4905 = 5.87 m ≈ 5.9 m
In reality, the ball will not reach this height because some energy is dissipated as heat (air resistance, friction) and sound.
Problem 3: A steel wire of length 4.0 m and diameter 1.0 mm supports a lift cage of mass 200 kg. The Young modulus of steel is 200 GPa.
(a) Calculate the stress in the wire. A = π(0.50 × 10⁻³)² = 7.854 × 10⁻⁷ m² F = 200 × 9.81 = 1962 N σ = F/A = 1962 / 7.854 × 10⁻⁷ = 2.50 × 10⁹ Pa = 2.50 GPa
(b) Calculate the strain. ε = σ/E = 2.50 × 10⁹ / 200 × 10⁹ = 0.0125
(c) Calculate the extension. ΔL = εL = 0.0125 × 4.0 = 0.050 m = 50 mm
(d) Calculate the elastic potential energy stored. E_stored = ½Fx = ½ × 1962 × 0.050 = 49.1 J
Reality check: The stress here (2.50 GPa) exceeds the UTS of most steels (typically 400–550 MPa). In practice, the wire would break. Real lift systems use much thicker cables. Always check whether your calculated stress is realistic.
Problem 4: A hollow steel sphere has an outer radius of 0.15 m and a wall thickness of 5.0 mm. The density of steel is 7800 kg m⁻³. Will it float in water?
Step 1 — Volume of steel: Outer volume = (4/3)π(0.15)³ = 1.414 × 10⁻² m³ Inner radius = 0.15 − 0.005 = 0.145 m Inner volume = (4/3)π(0.145)³ = 1.278 × 10⁻² m³ Volume of steel = 1.414 × 10⁻² − 1.278 × 10⁻² = 1.36 × 10⁻³ m³
Step 2 — Mass of sphere: m = ρV = 7800 × 1.36 × 10⁻³ = 10.6 kg
Step 3 — Average density: ρ_avg = m / V_outer = 10.6 / 1.414 × 10⁻² = 750 kg m⁻³
Since 750 < 1000 (water), the sphere floats. Fraction submerged = 750/1000 = 75%.
Problem 5: Describe an experiment to determine which of two metal wires (copper and steel) has the greater Young modulus.
Answer structure:
Key points for full marks:
Problem 6: A student measures the following for a copper wire:
Calculate the Young modulus and its percentage uncertainty.
Young modulus: A = π(0.24 × 10⁻³)² = 1.810 × 10⁻⁷ m² E = FL/(AΔL) = (30 × 2.50) / (1.810 × 10⁻⁷ × 1.5 × 10⁻³) = 75 / (2.715 × 10⁻¹⁰) = 2.76 × 10¹¹ Pa ≈ 276 GPa
Percentage uncertainties:
| Quantity | Value | Uncertainty | % uncertainty | Notes |
|---|---|---|---|---|
| Force F | 30 N | ±0.01 N | 0.03% | Negligible |
| Length L | 2.50 m | ±0.001 m | 0.04% | Negligible |
| Diameter d | 0.48 mm | ±0.02 mm | 4.17% | Doubled for area = 8.33% |
| Extension ΔL | 1.5 mm | ±0.1 mm | 6.67% | Largest single contribution |
Total % uncertainty in E = 0.03 + 0.04 + 8.33 + 6.67 = 15.1%
E = 276 ± 42 GPa (the accepted value of 130 GPa is well outside this range, indicating significant systematic error — likely in the diameter measurement).
Problem 7: An aerospace engineer needs to select a material for a landing gear component that must:
| Material | UTS (MPa) | E (GPa) | Density (kg m⁻³) | Toughness | Behaviour |
|---|---|---|---|---|---|
| Mild steel | 500 | 200 | 7800 | High | Ductile, tough |
| Al alloy | 450 | 70 | 2700 | Moderate | Ductile |
| Ti alloy | 900 | 110 | 4500 | Very high | Ductile, very tough |
| CFRP | 600 | 150 | 1600 | Low | Brittle (fails suddenly) |
Analysis:
Problem 8: A bungee cord has an unstretched length of 15.0 m and behaves like a spring with k = 50 N m⁻¹ for extensions up to 20 m. A person of mass 70 kg jumps from a bridge.
(a) How far does the person fall before the cord starts to stretch? The person falls 15.0 m (the natural length of the cord) before it begins to extend.
(b) When the cord has extended by 12.0 m, what is the net force on the person? Weight = mg = 70 × 9.81 = 686.7 N (downward) Tension = kx = 50 × 12.0 = 600 N (upward) Net force = 686.7 − 600 = 86.7 N downward
(c) What is the extension at equilibrium? At equilibrium: kx = mg → x = mg/k = 686.7/50 = 13.7 m Total distance = 15.0 + 13.7 = 28.7 m
(d) Using energy conservation, find the maximum extension (lowest point). At the lowest point: mgh = ½kx² where h = 15.0 + x 70 × 9.81 × (15.0 + x) = ½ × 50 × x² 686.7(15.0 + x) = 25x² 25x² − 686.7x − 10 300.5 = 0
Using the quadratic formula: x = (686.7 + √(686.7² + 4 × 25 × 10 300.5)) / (2 × 25) x = (686.7 + √(471 597 + 1 030 050)) / 50 x = (686.7 + 1225.4) / 50 = 38.2 m
Total distance fallen = 15.0 + 38.2 = 53.2 m
Exam insight: Part (d) is the hardest because students must recognise that the gravitational PE lost equals the elastic PE gained over the full distance (15.0 + x), not just the extension x. Setting up the energy equation correctly is worth most of the marks.
graph TD
A["Read the question\nIdentify known quantities"] --> B["Convert ALL units to SI\nmm to m, g to kg, etc."]
B --> C["Identify which equation(s)\nare needed"]
C --> D{"Multiple steps?"}
D -- Yes --> E["Solve step by step\nLabel intermediate answers"]
D -- No --> F["Substitute and solve"]
E --> G["Check: Are units correct?\nIs the magnitude sensible?"]
F --> G
G --> H["Round to appropriate s.f.\n(usually 2 or 3)"]
Before submitting your answer, check:
Edexcel 9PH0 Topic 4 — Materials, synoptic problem-solving is the integrative end-point of the topic: students combine density, fluid pressure and upthrust, Hooke's law, stress, strain, Young modulus, elastic and plastic deformation, and material-property selection within a single multi-step problem (refer to the official Pearson Edexcel specification document for exact wording). Topic 4 is examined principally on Paper 1, but materials-style synoptic items reappear on Paper 3, which is designed around AO3 problem-solving across topics. The Edexcel formula booklet provides Eel=21FΔL and p=hρg, but does not state ρ=m/V, σ=F/A, ε=ΔL/L or E=σ/ε — these must be memorised. Graders reward candidates who write each definition explicitly before substituting numbers.
Question (12 marks):
A new pedestrian footbridge is to be supported by two parallel steel cables of length L=24.0 m. Each cable must safely carry a maximum static load of F=8.5×104 N without exceeding 60% of the steel's yield stress. The steel has yield stress σy=2.50×108 Pa, density ρs=7850 kg m⁻³, and Young modulus E=2.10×1011 Pa.
(a) Determine the minimum cable diameter consistent with the safety criterion. (4)
(b) Calculate the cable's extension under the maximum load, using the diameter from (a). (3)
(c) Calculate the elastic strain energy stored in one fully loaded cable. (2)
(d) The cable hangs vertically below the bridge deck during installation. Show whether its self-weight contributes significantly (>5%) to the working stress at the upper attachment point. (3)
Solution with mark scheme:
(a) Step 1 — set the working stress.
Working stress σw=0.60×σy=0.60×2.50×108=1.50×108 Pa.
M1 — explicit application of the 60% safety factor; candidates who skip this step and design to the full yield stress lose this mark and propagate the error.
Step 2 — relate stress to cross-sectional area.
σ=F/A⟹A=F/σw=8.5×104/1.50×108=5.67×10−4 m².
M1 — correct rearrangement and substitution.
Step 3 — convert area to diameter.
A=πd2/4⟹d=4A/π=4×5.67×10−4/π=0.0269 m =26.9 mm.
M1 — correct use of A=πd2/4, not πd2 or πr2 with r=d.
A1 — final d≥26.9 mm (or 27 mm rounded up — accept the next standard manufactured size where stated).
(b) Step 1 — strain.
ε=σw/E=1.50×108/2.10×1011=7.14×10−4.
M1 — explicit use of ε=σ/E; candidates who try ΔL=FL/(AE) in one line and slip on a power of ten get partial credit only.
Step 2 — extension.
ΔL=εL=7.14×10−4×24.0=0.0171 m =17.1 mm.
M1 A1 — correct substitution and final value to 3 sf.
(c) Elastic strain energy from the formula booklet expression:
Eel=21FΔL=0.5×8.5×104×0.0171=727 J.
M1 A1 — direct substitution; both marks awarded for value in range 720–730 J.
(d) Step 1 — cable mass and weight.
Volume V=AL=5.67×10−4×24.0=1.36×10−2 m³.
Mass m=ρsV=7850×1.36×10−2=107 kg, weight W=mg=107×9.81=1.05×103 N.
M1 — correct application of m=ρV and W=mg with all SI units.
Step 2 — extra stress at the top of the cable.
σself=W/A=1.05×103/5.67×10−4=1.85×106 Pa.
M1 — recognising that the upper attachment carries the entire self-weight in addition to the load.
Step 3 — compare.
Fractional contribution =1.85×106/1.50×108=1.23%, which is well below the 5% threshold.
A1 — explicit numerical comparison and conclusion (statement that self-weight is not significant).
Total: 12 marks (M8 A4, split as shown).
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