Skip to content
Marlbridge

Practice Questions

AQA A-Level Physics: Mechanics and materials (7408) – Practice Questions

Original AQA A-Level Physics 7408 practice questions on mechanics and materials, with mark-by-mark worked answers and both required practicals.

Subject
Physics
Level
A LEVELS
Topic
Mechanics and materials
Updated

Aligned to AQA A Level Physics (7408), For first teaching 2015. Official specification .

Syllabus page (what it covers and how it is assessed): AQA A Level Physics.

Syllabus points this page covers

7408

  • 3.4.1 Force, energy and momentum
  • 3.4.2 Materials
  • 4 Mechanics and materials (whole topic)

Found an error? Report a correction.

Need help with this topic? Request a free trial class for A Level Physics (7408).

These are original questions written for Marlbridge, for revision and practice on this content. They are not reproduced past-paper questions, and they do not replicate the exam’s exact structure, question count or mark tariffs – examination boards hold copyright in their own papers. Use these alongside the official past papers from your board or school.

These questions cover section 3.4, Mechanics and materials, of AQA A-level Physics (7408), following the AQA AS and A-level Physics specification (7407/7408), version 1.4, for AS and A-level exams from June 2016 onwards. They span sub-sections 3.4.1.1 to 3.4.2.2, all of which are AS and A-level content, examined on A-level Paper 1 and assumed for Paper 2; the practical questions reflect Paper 3 Section A. Sections 3.9 to 3.13 are options: you study one, assessed in Paper 3 Section B. Take g = 9.81 m s⁻².

See the study guide, revision notes, course hub and printable checklist.

Questions

1. (a) State the difference between a scalar and a vector, giving one example of each. [2] (b) A rope pulls a crate with a force of 80 N at 35° above the horizontal. Calculate the horizontal and vertical components of this force. [2]

2. (a) A driver turns a steering wheel of diameter 0.38 m by applying two equal and opposite tangential forces of 15 N at opposite ends of a diameter. Calculate the moment of this couple. [2] (b) A uniform plank 4.0 m long and of weight 300 N rests on a single support 1.5 m from its left end. A vertical force F at the left end holds the plank horizontal. Calculate F and the force from the support. [4]

3. A cyclist accelerates uniformly from rest to 8.0 m s⁻¹ in 5.0 s, travels at constant speed for 12 s, then decelerates uniformly to rest in 4.0 s. (a) Calculate the initial acceleration. [1] (b) Calculate the total distance travelled. [3] (c) Calculate the average speed for the whole journey. [1]

4. In a free-fall experiment to find g, a steel ball is released from rest by an electromagnet and timed electronically over several heights h. A graph of h against t² is a straight line of gradient 4.87 m s⁻². (a) Show how the gradient is related to g and calculate g. [2] (b) The ball is released a short, constant time after the timer starts. State the type of error this causes and explain why a graph of √h against t would remove its effect on g. [3]

5. A ball is kicked from level ground at 18 m s⁻¹ at 40° above the horizontal. Ignore air resistance. (a) Calculate the time of flight. [3] (b) Calculate the maximum height reached. [2] (c) Calculate the horizontal range. [2] (d) Describe how air resistance would change the path. [2]

6. Explain why a skydiver falling from rest reaches a terminal speed. [3]

7. A car of mass 1100 kg tows a trailer of mass 400 kg along a level road. The driving force is 2400 N. Resistive forces are 300 N on the car and 150 N on the trailer. (a) Calculate the acceleration. [2] (b) Calculate the tension in the tow bar. [2] (c) State the Newton’s third law pair of the tow bar’s pull on the trailer. [1]

8. A 0.16 kg cricket ball travelling at 25 m s⁻¹ is hit straight back at 30 m s⁻¹. Contact lasts 8.0 ms. (a) Calculate the change in momentum. [2] (b) Calculate the average force on the ball. [1] (c) The force–time graph is a triangle. Calculate the peak force. [2] (d) Suggest why a padded glove reduces the force on a fielder’s hand when catching. [1]

9. A motor lifts a 2.4 kg load 1.5 m vertically at constant speed in 4.0 s. The input power is 18 W. (a) Calculate the useful output power using P = Fv. [3] (b) Calculate the efficiency as a percentage. [1]

10. Two trolleys, of mass 0.60 kg and 0.90 kg, are held at rest against a compressed spring between them. When released, the 0.60 kg trolley moves at 1.5 m s⁻¹. (a) Calculate the velocity of the 0.90 kg trolley. [2] (b) The spring was compressed by 0.050 m. Assuming all the elastic strain energy becomes kinetic energy, calculate the spring constant. [4]

11. A cyclist and bicycle, total mass 80 kg, freewheel from rest down a road, descending 12 m vertically over 150 m of road, and reach 11 m s⁻¹. Calculate the average resistive force. [4]

12. A student uses a 2.50 m length of copper wire of diameter 0.40 mm to find the Young modulus. (a) The wire has mass 2.8 g. Calculate the density of copper. [2] (b) A load of 30 N produces an extension of 5.0 mm, within the limit of proportionality. Calculate the Young modulus. [4] (c) Calculate the elastic strain energy stored at this load. [1] (d) Explain why a long, thin wire is used and why the diameter is measured at several places. [2] (e) The load is increased until the wire extends plastically. Describe what the force–extension graph shows when the load is then removed. [2]

Answers

1. (a) A scalar has magnitude only; a vector has magnitude and direction [1]. Example: mass (scalar), force (vector) [1]. (b) Horizontal = 80 cos 35° = 65.5 N [1]; vertical = 80 sin 35° = 45.9 N [1]. Examiner insight: Both examples are usually needed for the second mark; one correct example alone is not enough.

2. (a) Moment = one force × separation = 15 × 0.38 [1] = 5.7 N m [1]. (b) Weight acts at 2.0 m, so 0.5 m right of the support [1]. Moments about support: F × 1.5 = 300 × 0.5 [1], so F = 100 N [1]. Support force = 300 + 100 = 400 N [1]. Examiner insight: Moments about the support remove its unknown force; a consistent equation about another point still earns method marks.

3. (a) a = 8.0/5.0 = 1.6 m s⁻² [1]. (b) Areas: ½ × 8.0 × 5.0 = 20 m; 8.0 × 12 = 96 m [1]; ½ × 8.0 × 4.0 = 16 m [1]. Total = 132 m [1]. (c) 132 ÷ 21 = 6.3 m s⁻¹ [1]. Examiner insight: Error carried forward is normally allowed in (c), so a wrong total in (b) can still earn the average-speed mark.

4. (a) From rest, h = ½gt², so gradient = g/2 [1]; g = 2 × 4.87 = 9.74 m s⁻² [1]. (b) Systematic error [1]. Every measured time is too long by the same delay [1]. Since √h = √(g/2) × (t − delay), the √h–t graph is still a straight line of gradient √(g/2); the delay only moves the intercept, so g from the gradient is unaffected [1]. Examiner insight: “Systematic” alone earns one mark; the explanation must link the constant offset to the intercept, not the gradient.

5. (a) u_y = 18 sin 40° = 11.57 m s⁻¹ [1]. Back to launch height: 0 = u_y t − ½gt² [1], t = 2 × 11.57/9.81 = 2.36 s [1]. (b) At the top v_y = 0: h = u_y²/(2g) [1] = 6.82 m [1]. (c) uₓ = 18 cos 40° = 13.79 m s⁻¹ [1]; range = 13.79 × 2.36 = 32.5 m [1]. (d) Range and maximum height are smaller [1]; the path is asymmetric, with a steeper descent than ascent [1]. Examiner insight: Keep unrounded values between parts; rounding t to 2.4 s gives 33.1 m, which may lose the accuracy mark.

6. At first only weight acts, so the skydiver accelerates at g [1]. Air resistance increases with speed, so the resultant force and acceleration decrease [1]. When air resistance equals weight the resultant force is zero and speed is constant [1]. Examiner insight: “Forces balance” earns credit only if the answer names which forces: air resistance and weight.

7. (a) Resultant = 2400 − 300 − 150 = 1950 N [1]; a = 1950/1500 = 1.3 m s⁻² [1]. (b) For the trailer: T − 150 = 400 × 1.3 [1], T = 670 N [1]. (c) The trailer’s pull on the tow bar (and so on the car), 670 N backwards [1]. Examiner insight: A third-law partner must act on a different body; naming the trailer’s weight or friction scores zero.

8. (a) Taking the rebound direction as positive: Δp = 0.16 × (30 − (−25)) [1] = 8.8 N s [1]. (b) F = 8.8/0.0080 = 1100 N [1]. (c) Area = ½ × 0.0080 × F_peak = 8.8 [1], so F_peak = 2200 N [1]. (d) The padding increases the stopping time, so a smaller force gives the same change in momentum [1]. Examiner insight: Using 30 − 25 for the velocity change gives 0.80 N s and loses both marks in (a); direction matters.

9. (a) v = 1.5/4.0 = 0.375 m s⁻¹ [1]; F = mg = 2.4 × 9.81 = 23.5 N [1]; P = 23.5 × 0.375 = 8.83 W [1]. (b) 8.83/18 × 100 = 49% [1]. Examiner insight: At constant speed the lifting force equals the weight; no “ma” term is needed.

10. (a) Total momentum stays zero: 0.60 × 1.5 = 0.90v [1], so v = 1.0 m s⁻¹ in the opposite direction [1]. (b) Ek = ½ × 0.60 × 1.5² + ½ × 0.90 × 1.0² [1] = 1.125 J [1]. ½k(0.050)² = 1.125 [1], so k = 900 N m⁻¹ [1]. Examiner insight: The direction is required for the second mark in (a); velocity is a vector.

11. Ep lost = 80 × 9.81 × 12 = 9418 J [1]. Ek gained = ½ × 80 × 11² = 4840 J [1]. Work against resistance = 4578 J [1]. F = 4578/150 = 31 N [1]. Examiner insight: The resistive force acts along the road, so divide by 150 m, not the 12 m height.

12. (a) A = π(0.20 × 10⁻³)² = 1.257 × 10⁻⁷ m²; V = 3.14 × 10⁻⁷ m³ [1]. ρ = 2.8 × 10⁻³/3.14 × 10⁻⁷ = 8.9 × 10³ kg m⁻³ [1]. (b) Stress = 30/1.257 × 10⁻⁷ = 2.39 × 10⁸ Pa [1]. Strain = 5.0 × 10⁻³/2.50 = 2.0 × 10⁻³ [1]. E = stress/strain [1] = 1.2 × 10¹¹ Pa [1]. (c) ½ × 30 × 5.0 × 10⁻³ = 0.075 J [1]. (d) A long, thin wire gives a large enough extension to measure precisely [1]; the wire may not be uniform, so a mean diameter reduces uncertainty in the area [1]. (e) The unloading line is straight and parallel to the loading line [1], and does not return to zero: a permanent extension remains [1]. Examiner insight: Using the diameter as the radius makes the area four times too large and E four times too small, losing the accuracy marks.

Where marks are usually lost

  • Measuring a moment arm along the beam instead of perpendicular to the line of action.
  • Losing the sign of a rebound velocity, so the momentum change comes out far too small.
  • Rounding an intermediate time in a projectile question and missing the final accuracy mark.
  • Naming two forces on the same body as a Newton’s third law pair.
  • Treating terminal speed as “no forces acting” rather than zero resultant force.
  • Forgetting work done against resistive forces when applying energy conservation.
  • Describing the Young modulus graph method without saying the gradient of the straight section is used.

Next steps

Official syllabus

AQA AS and A-level Physics specification (7407/7408), version 1.4, July 2026, for AS and A-level exams June 2016 onwards, published by AQA. Section 3.4 Mechanics and materials.

Get free revision emails (optional)

Occasional emails with practice questions, worked explanations and links to free resources for the qualification and subjects you choose. No spam, and you can unsubscribe from any email. The free tools on this site never need an email.

Subjects (optional, up to 6)

Choose a qualification to see its subjects.

Related resources

Related articles

Studying this with a teacher

Working through Physics A LEVELS?

This page is free and stays free. If you would rather be taught it, Marlbridge runs Physics classes one-to-one and in small groups of up to 15, online in your own time zone. The first trial class is free. WhatsApp replies within an hour (8am–11pm Pakistan time, every day); email the same day.