Question Simulator

AS & A Level Physics (9702)

Superposition Banker

154 questions · about 5% of the marks we indexed · examined in 9 of 9 sessions.

Questions by year

2026

  • 2026 May/June · Paper 11 · Q271 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 11 · Q281 markDiffraction
  • 2026 May/June · Paper 11 · Q291 markInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 11 · Q301 markInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 12 · Q261 markDiffraction
  • 2026 May/June · Paper 12 · Q271 markDiffraction grating
  • 2026 May/June · Paper 12 · Q281 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 12 · Q291 markInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 13 · Q271 markInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 13 · Q281 markDiffraction grating
  • 2026 May/June · Paper 13 · Q291 markDiffraction grating
  • 2026 May/June · Paper 13 · Q301 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 14 · Q281 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 14 · Q291 markInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 14 · Q301 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 14 · Q311 markSuperposition principle & stationary waves
  • 2026 May/June · Paper 21 · Q3 (c(i), c(ii), c(iii))6 marksSuperposition principle & stationary waves
  • 2026 May/June · Paper 22 · Q3 (b(ii), c(ii))5 marksInterference & coherence (two-source / double slit)
  • 2026 May/June · Paper 23 · Q3 (a, b(i), b(ii), b(iii), b(iv), c(i), c(ii), d)14 marksDiffraction · Interference & coherence (two-source / double slit) · Superposition principle & stationary waves
  • 2026 May/June · Paper 24 · Q3 (a, b, c, d)8 marksSuperposition principle & stationary waves

2025

  • 2025 Oct/Nov · Paper 11 · Q281 markInterference & coherence (two-source / double slit)
  • 2025 Oct/Nov · Paper 11 · Q291 markSuperposition principle & stationary waves
  • 2025 Oct/Nov · Paper 11 · Q301 markDiffraction grating
  • 2025 Oct/Nov · Paper 12 · Q281 markDiffraction
  • 2025 Oct/Nov · Paper 12 · Q291 markDiffraction grating
  • 2025 Oct/Nov · Paper 12 · Q301 markSuperposition principle & stationary waves
  • 2025 Oct/Nov · Paper 12 · Q311 markInterference & coherence (two-source / double slit)
  • 2025 Oct/Nov · Paper 13 · Q281 markInterference & coherence (two-source / double slit)
  • 2025 Oct/Nov · Paper 13 · Q291 markSuperposition principle & stationary waves
  • 2025 Oct/Nov · Paper 13 · Q301 markDiffraction grating
  • 2025 Oct/Nov · Paper 14 · Q261 markDiffraction
  • 2025 Oct/Nov · Paper 14 · Q291 markSuperposition principle & stationary waves
  • 2025 Oct/Nov · Paper 14 · Q301 markDiffraction grating
  • 2025 Oct/Nov · Paper 14 · Q311 markInterference & coherence (two-source / double slit)
  • 2025 Oct/Nov · Paper 21 · Q4 (a, b(i), b(ii), b(iii))8 marksDiffraction · Diffraction grating
  • 2025 Oct/Nov · Paper 22 · Q4 (a, b, c)8 marksInterference & coherence (two-source / double slit)
  • 2025 Oct/Nov · Paper 23 · Q4 (a, b(i), b(ii), b(iii))8 marksDiffraction · Diffraction grating
  • 2025 Oct/Nov · Paper 24 · Q4 (a, b(i), b(iv))6 marksSuperposition principle & stationary waves
  • 2025 May/June · Paper 11 · Q291 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 11 · Q301 markDiffraction grating
  • 2025 May/June · Paper 11 · Q311 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 12 · Q241 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 12 · Q291 markDiffraction grating
  • 2025 May/June · Paper 12 · Q301 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 12 · Q311 markInterference & coherence (two-source / double slit)
  • 2025 May/June · Paper 13 · Q281 markInterference & coherence (two-source / double slit)
  • 2025 May/June · Paper 13 · Q291 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 13 · Q301 markDiffraction
  • 2025 May/June · Paper 13 · Q311 markInterference & coherence (two-source / double slit)
  • 2025 May/June · Paper 14 · Q251 markSuperposition principle & stationary waves
  • 2025 May/June · Paper 14 · Q261 markDiffraction
  • 2025 May/June · Paper 14 · Q271 markInterference & coherence (two-source / double slit)
  • 2025 May/June · Paper 14 · Q281 markDiffraction grating
  • 2025 May/June · Paper 21 · Q4 (a, b(i), b(ii))8 marksInterference & coherence (two-source / double slit) · Superposition principle & stationary waves
  • 2025 May/June · Paper 22 · Q3 (b(ii), c)3 marksInterference & coherence (two-source / double slit) · Superposition principle & stationary waves
  • 2025 May/June · Paper 23 · Q6 (a, b(i), b(ii), b(iii))8 marksDiffraction · Diffraction grating
  • 2025 May/June · Paper 24 · Q4 (b(i), b(ii), b(iii), b(iv))8 marksInterference & coherence (two-source / double slit)

2024

  • 2024 Oct/Nov · Paper 11 · Q271 markInterference & coherence (two-source / double slit)
  • 2024 Oct/Nov · Paper 11 · Q281 markSuperposition principle & stationary waves
  • 2024 Oct/Nov · Paper 11 · Q301 markDiffraction grating
  • 2024 Oct/Nov · Paper 12 · Q281 markSuperposition principle & stationary waves
  • 2024 Oct/Nov · Paper 12 · Q291 markDiffraction
  • 2024 Oct/Nov · Paper 12 · Q301 markDiffraction grating
  • 2024 Oct/Nov · Paper 12 · Q311 markSuperposition principle & stationary waves
  • 2024 Oct/Nov · Paper 13 · Q281 markSuperposition principle & stationary waves
  • 2024 Oct/Nov · Paper 13 · Q291 markInterference & coherence (two-source / double slit)
  • 2024 Oct/Nov · Paper 13 · Q301 markDiffraction
  • 2024 Oct/Nov · Paper 21 · Q6 (a(i), a(ii), b(i), b(ii), b(iii))9 marksInterference & coherence (two-source / double slit)
  • 2024 Oct/Nov · Paper 22 · Q4 (b(i), b(ii), b(iii))6 marksSuperposition principle & stationary waves
  • 2024 Oct/Nov · Paper 23 · Q5 (a(i), a(ii), a(iii))4 marksSuperposition principle & stationary waves
  • 2024 May/June · Paper 11 · Q261 markOfficial paper ↗Diffraction grating
  • 2024 May/June · Paper 11 · Q301 markOfficial paper ↗Interference & coherence (two-source / double slit)
  • 2024 May/June · Paper 12 · Q221 markDiffraction
  • 2024 May/June · Paper 12 · Q231 markSuperposition principle & stationary waves
  • 2024 May/June · Paper 12 · Q261 markDiffraction grating
  • 2024 May/June · Paper 12 · Q271 markSuperposition principle & stationary waves
  • 2024 May/June · Paper 12 · Q281 markInterference & coherence (two-source / double slit)
  • 2024 May/June · Paper 13 · Q271 markSuperposition principle & stationary waves
  • 2024 May/June · Paper 13 · Q281 markDiffraction
  • 2024 May/June · Paper 13 · Q291 markDiffraction grating
  • 2024 May/June · Paper 21 · Q5 (a, b, c, d, e)8 marksOfficial paper ↗Superposition principle & stationary waves
  • 2024 May/June · Paper 22 · Q6 (a, b(ii))5 marksDiffraction grating
  • 2024 May/June · Paper 23 · Q4 (d)3 marksInterference & coherence (two-source / double slit)

2023

  • 2023 Oct/Nov · Paper 11 · Q251 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 11 · Q261 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 11 · Q271 markDiffraction
  • 2023 Oct/Nov · Paper 11 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 Oct/Nov · Paper 11 · Q291 markDiffraction grating
  • 2023 Oct/Nov · Paper 12 · Q251 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 12 · Q261 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 12 · Q271 markDiffraction
  • 2023 Oct/Nov · Paper 12 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 Oct/Nov · Paper 12 · Q291 markDiffraction grating
  • 2023 Oct/Nov · Paper 13 · Q251 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 13 · Q261 markSuperposition principle & stationary waves
  • 2023 Oct/Nov · Paper 13 · Q271 markDiffraction
  • 2023 Oct/Nov · Paper 13 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 Oct/Nov · Paper 13 · Q291 markDiffraction grating
  • 2023 Oct/Nov · Paper 21 · Q4 (a, b, c(i), c(ii), d)9 marksDiffraction · Interference & coherence (two-source / double slit) · Superposition principle & stationary waves
  • 2023 Oct/Nov · Paper 22 · Q5 (b, c(i), c(ii))6 marksDiffraction · Diffraction grating
  • 2023 Oct/Nov · Paper 23 · Q5 (a(i), a(ii), b(i))5 marksInterference & coherence (two-source / double slit)
  • 2023 May/June · Paper 11 · Q251 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 11 · Q261 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 11 · Q271 markDiffraction
  • 2023 May/June · Paper 11 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 May/June · Paper 11 · Q291 markDiffraction grating
  • 2023 May/June · Paper 12 · Q251 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 12 · Q261 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 12 · Q271 markDiffraction
  • 2023 May/June · Paper 12 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 May/June · Paper 12 · Q291 markDiffraction grating
  • 2023 May/June · Paper 13 · Q251 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 13 · Q261 markSuperposition principle & stationary waves
  • 2023 May/June · Paper 13 · Q271 markDiffraction
  • 2023 May/June · Paper 13 · Q281 markInterference & coherence (two-source / double slit)
  • 2023 May/June · Paper 13 · Q291 markDiffraction grating
  • 2023 May/June · Paper 21 · Q5 (b(i), b(ii), c(i), c(ii))6 marksInterference & coherence (two-source / double slit)
  • 2023 May/June · Paper 22 · Q5 (b(i), b(ii), b(iii))4 marksSuperposition principle & stationary waves
  • 2023 May/June · Paper 23 · Q4 (d(i), d(ii), d(iii))6 marksSuperposition principle & stationary waves

2022

  • 2022 Oct/Nov · Paper 11 · Q261 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 11 · Q271 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 11 · Q281 markDiffraction
  • 2022 Oct/Nov · Paper 11 · Q291 markInterference & coherence (two-source / double slit)
  • 2022 Oct/Nov · Paper 11 · Q301 markDiffraction grating
  • 2022 Oct/Nov · Paper 12 · Q261 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 12 · Q271 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 12 · Q281 markDiffraction
  • 2022 Oct/Nov · Paper 12 · Q291 markInterference & coherence (two-source / double slit)
  • 2022 Oct/Nov · Paper 12 · Q301 markDiffraction grating
  • 2022 Oct/Nov · Paper 13 · Q251 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 13 · Q261 markSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 13 · Q271 markDiffraction
  • 2022 Oct/Nov · Paper 13 · Q281 markInterference & coherence (two-source / double slit)
  • 2022 Oct/Nov · Paper 13 · Q291 markDiffraction grating
  • 2022 Oct/Nov · Paper 21 · Q4 (c(i), c(ii))5 marksSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 22 · Q5 (a, b(i), b(ii))6 marksSuperposition principle & stationary waves
  • 2022 Oct/Nov · Paper 23 · Q4 (d(i), d(ii))3 marksSuperposition principle & stationary waves
  • 2022 May/June · Paper 11 · Q261 markSuperposition principle & stationary waves
  • 2022 May/June · Paper 11 · Q271 markSuperposition principle & stationary waves
  • 2022 May/June · Paper 11 · Q281 markDiffraction
  • 2022 May/June · Paper 11 · Q291 markInterference & coherence (two-source / double slit)
  • 2022 May/June · Paper 11 · Q301 markDiffraction grating
  • 2022 May/June · Paper 12 · Q271 markSuperposition principle & stationary waves
  • 2022 May/June · Paper 12 · Q281 markDiffraction
  • 2022 May/June · Paper 12 · Q291 markInterference & coherence (two-source / double slit)
  • 2022 May/June · Paper 12 · Q301 markDiffraction grating
  • 2022 May/June · Paper 13 · Q271 markSuperposition principle & stationary waves
  • 2022 May/June · Paper 13 · Q281 markSuperposition principle & stationary waves
  • 2022 May/June · Paper 13 · Q291 markDiffraction
  • 2022 May/June · Paper 13 · Q301 markInterference & coherence (two-source / double slit)
  • 2022 May/June · Paper 13 · Q311 markDiffraction grating
  • 2022 May/June · Paper 21 · Q5 (a, b, c, d)8 marksSuperposition principle & stationary waves
  • 2022 May/June · Paper 22 · Q5 (a, b(i), b(ii), c, d, e)11 marksInterference & coherence (two-source / double slit)
  • 2022 May/June · Paper 23 · Q5 (b(iii), b(iv))6 marksDiffraction grating

References only, not question text. Open Official paper ↗ where Cambridge publishes the paper, or see the official Cambridge past-papers page; for other papers, ask your school. “Paper 42” means Paper 4, variant 2.

Practice questions

Original questions written by HomiLabs in the style of the exam, with answers and mark schemes. They are not Cambridge past paper questions and have not been reviewed by Cambridge. Try each one before opening the answer.

Q1Superposition principle & stationary waves · Core · Paper 1 style · 1 mark
  1. (a) [1]
Show answer
  1. (a) C 60 m s⁻¹
    Node-to-node distance = λ/2, so λ = 0.50 m and v = fλ = 120 × 0.50 = 60 m s⁻¹. 30 m s⁻¹ wrongly takes λ = 0.25 m.
Q2Superposition principle & stationary waves · Core · Paper 2 style · 6 marks
  1. (a) State the principle of superposition. [2]
  2. (b) State two differences between a stationary wave and a progressive wave. [2]
  3. (c) Explain how a stationary wave is formed on a stretched string fixed at both ends. [2]
Show answer
  1. (a) When two or more waves meet at a point, the resultant displacement is the sum of the individual displacements.
    B1: waves meet/overlap at a point; B1: resultant displacement = (vector) sum of individual displacements.
  2. (b) Stationary: no net energy transfer; amplitude varies with position (nodes and antinodes); points between adjacent nodes are in phase.
    B1 each for any two: stationary wave transfers no energy (progressive does); amplitude varies from zero at nodes to maximum at antinodes (progressive: same amplitude everywhere); all points between two adjacent nodes vibrate in phase (progressive: phase changes continuously with distance); wave profile does not move along.
  3. (c) Waves travel along the string and reflect at the fixed ends; the incident and reflected waves, of the same frequency and speed, travelling in opposite directions, superpose.
    B1: wave reflected at the end; B1: two waves of same frequency/wavelength (and similar amplitude) travelling in opposite directions superpose/interfere.
Q3Superposition principle & stationary waves · Core · Paper 2 style · 5 marks

A plastic pipe of length 0.68 m is open at both ends. Air in the pipe is made to vibrate. Speed of sound = 340 m s⁻¹. Ignore end corrections.

  1. (a) State where the nodes and antinodes are when the pipe sounds its lowest note. [2]
  2. (b) Calculate the frequency of the lowest note. [2]
  3. (c) Calculate the frequency of the next higher note the pipe can produce. [1]
Show answer
  1. (a) Antinodes at both open ends; one node at the centre.
    B1: antinode at each open end; B1: single node in the middle.
  2. (b) 250 Hz
    Length = λ/2 → λ = 1.36 m (M1); f = 340/1.36 = 250 Hz (A1).
  3. (c) 500 Hz
    Two nodes, λ = 0.68 m → f = 500 Hz (A1).
Q4Superposition principle & stationary waves · Standard · Paper 2 style · 5 marks

A string of length 1.20 m is fixed at both ends and made to vibrate by a vibration generator. When the frequency is 150 Hz a stationary wave with three loops (three antinodes) is formed.

  1. (a) Calculate the wavelength of the waves on the string. [1]
  2. (b) Calculate the speed of the waves on the string. [1]
  3. (c) Determine the lowest frequency at which a stationary wave can be formed on this string, and the frequency that gives four loops. [2]
  4. (d) State the number of nodes, including the ends, when there are four loops. [1]
Show answer
  1. (a) 0.80 m
    Three loops = 3 × λ/2 = 1.20 m → λ = 0.80 m (A1).
  2. (b) 120 m s⁻¹
    v = fλ = 150 × 0.80 = 120 m s⁻¹ (A1).
  3. (c) 50 Hz and 200 Hz
    Fundamental: λ = 2.40 m, f = 120/2.40 = 50 Hz (A1); four loops: λ = 0.60 m, f = 200 Hz (A1).
  4. (d) 5
    B1: four loops have nodes at both ends plus three between = 5.
Q5Superposition principle & stationary waves · Standard · Paper 2 style · 6 marks

A vertical tube, open at the top, has its lower end in water so that the length of the air column can be changed. A tuning fork of frequency 512 Hz is held over the top. Loud sounds are heard when the air column has lengths 0.165 m and 0.505 m (the first two resonances).

  1. (a) Explain why a loud sound is heard at certain lengths of the air column. [2]
  2. (b) Calculate the speed of sound in the tube. [2]
  3. (c) The antinode at the open end is slightly outside the tube. Use the data to find how far outside the tube it is. [2]
Show answer
  1. (a) A stationary wave forms in the air column (resonance) with a node at the water surface and an antinode near the open end.
    B1: sound reflected at water surface forms stationary wave; B1: resonance when the column length allows a node at the closed end and antinode at the open end (natural frequency = fork frequency).
  2. (b) 348 m s⁻¹
    Difference between successive resonance lengths = λ/2 (M1): λ = 2 × 0.340 = 0.680 m; v = 512 × 0.680 = 348 m s⁻¹ (A1).
  3. (c) 0.005 m (about 5 mm)
    First resonance: l₁ + e = λ/4 (M1); e = 0.170 − 0.165 = 0.005 m (A1).
Q6Superposition principle & stationary waves · Standard · Paper 1 style · 1 mark
  1. (a) Two points P and Q on a stationary wave lie between the same pair of adjacent nodes. P is at the antinode and Q is close to one of the nodes. What is the phase difference between the oscillations of P and Q? [1]
Show answer
  1. (a) A 0
    All points between two adjacent nodes oscillate in phase (with different amplitudes). A phase difference that depends on distance is true for a progressive wave, not a stationary wave.
Q7Superposition principle & stationary waves · Standard · Paper 2 style · 6 marks

A stationary wave of wavelength 0.60 m is set up on a long rope. One fixed end is at x = 0, which is a node. Points P, Q and R on the rope are at x = 0.15 m, x = 0.20 m and x = 0.45 m.

  1. (a) State the positions of all the nodes between x = 0 and x = 0.90 m inclusive. [1]
  2. (b) State the phase difference between the oscillations of (i) P and Q, (ii) P and R. [2]
  3. (c) At one instant P is at its maximum upward displacement. Describe the displacements of Q and R at this instant. [2]
  4. (d) State the displacement of every point on the rope a quarter of a period later. [1]
Show answer
  1. (a) x = 0, 0.30 m, 0.60 m, 0.90 m
    B1: nodes every λ/2 = 0.30 m, starting at the fixed end.
  2. (b) (i) 0; (ii) 180° (π rad)
    B1: P (x = 0.15 m) and Q (x = 0.20 m) are in the same loop → in phase; B1: R (x = 0.45 m) is in the adjacent loop → antiphase.
  3. (c) Q is displaced upwards by a smaller amount (it is at its own maximum); R is at its maximum downward displacement.
    B1: Q upward, smaller amplitude than P (P is at an antinode); B1: R maximum displacement downward (R is also at an antinode, opposite phase).
  4. (d) Zero (the rope is momentarily straight).
    B1: all points pass through equilibrium at the same time.
Q8Superposition principle & stationary waves · Standard · Paper 3 style · 7 marks

A string passes over a pulley and is kept under constant tension by a hanging mass. A vibration generator drives one end. The vibrating length L of the string is changed and the frequency f of the fundamental mode (one loop) is found each time:L = 0.400 m, f = 61 HzL = 0.500 m, f = 47 HzL = 0.600 m, f = 40 HzL = 0.700 m, f = 35 HzL = 0.800 m, f = 30 HzL = 0.900 m, f = 26 Hz

  1. (a) Theory suggests f = v/(2L), where v is the speed of waves on the string. State the graph that should be plotted to give a straight line through the origin. [1]
  2. (b) Calculate 1/L for each reading, with an appropriate unit. [1]
  3. (c) The best-fit line through the origin has gradient 24.0 m s⁻¹. Determine the speed of the waves on the string. [1]
  4. (d) Suggest two difficulties in deciding when the string is vibrating at its fundamental frequency, and an improvement for each. [4]
Show answer
  1. (a) f against 1/L
    B1: f on y-axis against 1/L on x-axis (or L against 1/f).
  2. (b) 1/L / m⁻¹: 2.50, 2.00, 1.67, 1.43, 1.25, 1.11
    B1: all correct with unit m⁻¹ (3 s.f.).
  3. (c) 48.0 m s⁻¹
    v = 2 × gradient = 2 × 24.0 = 48.0 m s⁻¹ (A1).
  4. (d) e.g. amplitude changes slowly near resonance so the peak is hard to judge — approach from above and below and average; the vibrations are fast and hard to see — use a strobe lamp or a dark background with bright lighting; the generator end is not a perfect node — measure L between two nodes.
    B1 + B1: two distinct difficulties; B1 + B1: matching specific improvements (repeat from both sides and average; use stroboscope; measure between nodes, not from the generator; use a fine-tune frequency control/digital meter).
Q9Superposition principle & stationary waves · Challenge · Paper 2 style · 7 marks

A microwave transmitter faces a flat metal plate. A detector is moved along the line between them. The distance between the first and the tenth minimum readings (9 intervals) is 13.5 cm. Speed of electromagnetic waves = 3.00 × 10⁸ m s⁻¹.

  1. (a) Explain why the detector reading rises and falls as it is moved. [2]
  2. (b) Calculate the wavelength and the frequency of the microwaves. [3]
  3. (c) The readings at the minima are not zero. Suggest why, and explain why the minima are smaller close to the plate. [2]
Show answer
  1. (a) Incident and reflected microwaves superpose to form a stationary wave; maxima at antinodes and minima at nodes.
    B1: reflected wave superposes with incident wave (same frequency, opposite directions); B1: stationary wave with nodes (minima) and antinodes (maxima).
  2. (b) λ = 0.030 m; f = 1.0 × 10¹⁰ Hz
    9 node spacings = 13.5 cm → node spacing 1.50 cm = λ/2 (M1); λ = 0.030 m (A1); f = c/λ = 1.0 × 10¹⁰ Hz (A1).
  3. (c) The reflected wave has a smaller amplitude than the incident wave (some energy absorbed/spread out), so cancellation is incomplete; near the plate the two amplitudes are more nearly equal.
    B1: amplitudes of incident and reflected waves not equal → no complete cancellation; B1: reflected wave spreads out with distance from the plate, so the amplitudes are closest near the plate.
Q10Superposition principle & stationary waves · Challenge · Paper 2 style · 6 marks

A guitar string of vibrating length 0.65 m sounds its fundamental frequency of 196 Hz.

  1. (a) Calculate the speed of the waves on the string. [2]
  2. (b) The player presses the string against a fret so that the vibrating length is shorter and the fundamental frequency becomes 247 Hz. The tension does not change. Calculate the new vibrating length. [2]
  3. (c) The string makes a sound wave in air of frequency 247 Hz. The speed of sound in air is 340 m s⁻¹. Calculate the wavelength of this sound and explain why it differs from the wavelength of the wave on the string. [2]
Show answer
  1. (a) 255 m s⁻¹
    Fundamental: λ = 2L = 1.30 m (M1); v = 196 × 1.30 = 255 m s⁻¹ (A1).
  2. (b) 0.516 m
    Same wave speed (M1); L = v/(2f) = 255/(2 × 247) = 0.516 m (A1).
  3. (c) 1.38 m; the frequency is the same but the wave speed in air is different.
    λ = 340/247 = 1.38 m (A1); B1: frequency is fixed by the source; speed in air differs from speed on string, so λ = v/f differs.
Q11Superposition principle & stationary waves · Challenge · Paper 1 style · 1 mark
  1. (a) [1]
Show answer
  1. (a) A 240 Hz
    A closed pipe has a node at the closed end and an antinode at the open end, so only odd multiples of the fundamental occur: 120, 360, 600, 840 Hz, … 240 Hz is an even multiple, which needs antinodes at both ends (an open pipe).
Q12Interference & coherence (two-source / double slit) · Core · Paper 2 style · 4 marks
  1. (a) Explain what is meant by coherent sources. [1]
  2. (b) Explain why two separate light bulbs do not produce a visible interference pattern, whereas light from a single laser passing through two narrow slits does. [2]
  3. (c) State one other condition needed for the dark fringes in a two-source pattern to be completely dark. [1]
Show answer
  1. (a) Sources with a constant phase difference (and so the same frequency).
    B1: constant phase difference.
  2. (b) Light from separate bulbs is emitted randomly, so the phase difference changes rapidly — the pattern changes too fast to see; the two slits are illuminated by the same wavefront, so the two sources are coherent.
    B1: bulbs are not coherent — phase difference varies randomly/rapidly; B1: slits take light from the same source/wavefront, so constant phase difference.
  3. (c) The two waves must have equal amplitudes at the point (and be polarised in the same plane).
    B1: equal amplitude (accept same polarisation for unpolarised/transverse case).
Q13Interference & coherence (two-source / double slit) · Core · Paper 1 style · 1 mark
  1. (a) In a double-slit experiment with light, which single change increases the separation of the bright fringes on the screen? [1]
Show answer
  1. (a) D using slits that are closer together
    x = λD/a, so x increases when the slit separation a decreases. Blue light has a shorter wavelength than red, so it reduces the fringe spacing; moving the screen closer reduces D.
Q14Interference & coherence (two-source / double slit) · Core · Paper 2 style · 4 marks

Two dippers S₁ and S₂ in a ripple tank vibrate in phase and produce water waves of wavelength 2.4 cm. Point P on the water surface is 15.6 cm from S₁ and 21.6 cm from S₂.

  1. (a) Calculate the path difference at point P and state, with a reason, whether P is a point of maximum or minimum amplitude. [2]
  2. (b) Point Q is 18.0 cm from S₁ and 22.8 cm from S₂. State whether Q is a maximum or a minimum. [1]
  3. (c) The dippers are now adjusted so that they vibrate in antiphase. State what is now observed at P. [1]
Show answer
  1. (a) 6.0 cm = 2.5λ, so minimum (destructive interference).
    B1: 21.6 − 15.6 = 6.0 cm = 2.5λ; B1: odd number of half-wavelengths → waves arrive in antiphase → minimum.
  2. (b) Maximum (path difference 4.8 cm = 2λ).
    B1: 4.8/2.4 = 2 whole wavelengths → in phase → maximum.
  3. (c) P becomes a maximum.
    B1: extra phase difference of 180° turns the minimum into a maximum.
Q15Interference & coherence (two-source / double slit) · Standard · Paper 2 style · 5 marks

Light from a laser passes through two narrow parallel slits 0.45 mm apart. An interference pattern is seen on a screen 2.40 m from the slits. The distance from the centre of the first bright fringe to the centre of the eleventh bright fringe is 32.0 mm.

  1. (a) Calculate the fringe separation. [1]
  2. (b) Calculate the wavelength of the light. [2]
  3. (c) The light is replaced by light of wavelength 450 nm. Calculate the new fringe separation. [1]
  4. (d) State and explain one reason why the width of 11 fringes is measured rather than the width of one. [1]
Show answer
  1. (a) 3.2 mm
    11 bright fringes have 10 spacings: 32.0/10 = 3.2 mm (B1).
  2. (b) 600 nm
    λ = ax/D (M1) = 0.45 × 10⁻³ × 3.2 × 10⁻³/2.40 = 6.0 × 10⁻⁷ m (A1).
  3. (c) 2.4 mm
    x = λD/a = 2.4 mm (A1).
  4. (d) It reduces the percentage uncertainty in the fringe separation.
    B1: the absolute uncertainty in reading the ruler is shared over 10 spacings, so % uncertainty is smaller.
Q16Interference & coherence (two-source / double slit) · Standard · Paper 2 style · 5 marks

On a school sports ground, two loudspeakers 3.0 m apart are connected to the same signal generator and emit sound of frequency 680 Hz in phase. A student walks along a line parallel to the line joining the speakers and 12 m from it, and hears loud and quiet points. Speed of sound = 340 m s⁻¹.

  1. (a) Calculate the wavelength of the sound. [1]
  2. (b) State the path difference from the two loudspeakers to the first quiet point next to the central loud point. [1]
  3. (c) Estimate the distance the student walks between adjacent loud points. [2]
  4. (d) Suggest why the sound at the quiet points is not completely silent. [1]
Show answer
  1. (a) 0.50 m
    λ = v/f = 340/680 = 0.50 m (A1).
  2. (b) 0.25 m
    Half a wavelength = 0.25 m (B1).
  3. (c) 2.0 m
    x = λD/a (M1) = 0.50 × 12/3.0 = 2.0 m (A1). (The angle is small, about 10°, so the formula is a fair estimate.)
  4. (d) Sound reflects from the ground and nearby buildings, and the waves from the two loudspeakers do not have equal amplitudes at the point.
    B1: amplitudes unequal (different distances) / reflections from surroundings add other waves.
Q17Interference & coherence (two-source / double slit) · Standard · Paper 1 style · 1 mark
  1. (a) Two coherent sources emit waves of wavelength λ exactly in antiphase. At a point P the path difference from the two sources is 2λ. What is observed at P? [1]
Show answer
  1. (a) B a minimum, because the waves arrive in antiphase
    A path difference of 2λ adds no extra phase difference, so the waves keep their original 180° phase difference and cancel. A ignores the antiphase sources. D is wrong: a constant phase difference (180°) still gives a stable pattern.
Q18Interference & coherence (two-source / double slit) · Standard · Paper 2 style · 5 marks

A double slit with slit separation 0.30 mm is illuminated with white light. A screen is placed 1.5 m from the slits.

  1. (a) Describe the pattern seen on the screen when white light is used. [3]
  2. (b) Calculate the distance on the screen between the red (700 nm) and violet (400 nm) edges of the first-order bright fringe. [2]
Show answer
  1. (a) A white central fringe; on each side, coloured fringes with violet/blue nearest the centre and red furthest; fringes become blurred and overlap further out.
    B1: central fringe white (all wavelengths have zero path difference); B1: other bright fringes are spectra, violet edge nearer centre, red outer edge; B1: few fringes visible as orders overlap / pattern fades to white.
  2. (b) 1.5 mm
    x = λD/a for each: red 3.5 mm, violet 2.0 mm (M1); difference 1.5 mm (A1).
Q19Interference & coherence (two-source / double slit) · Standard · Paper 3 style · 6 marks

A student shines a laser through a double slit. She records:width of 6 fringe spacings w = 14 ± 1 mmslit-to-screen distance D = 1.85 ± 0.01 mslit separation a = 0.50 ± 0.02 mm

  1. (a) Calculate the wavelength of the laser light. [2]
  2. (b) Calculate the percentage uncertainty in the wavelength. [2]
  3. (c) Hence state the wavelength with its absolute uncertainty. [1]
  4. (d) Suggest one change to the procedure that would most reduce the uncertainty. [1]
Show answer
  1. (a) 6.3 × 10⁻⁷ m
    x = 14/6 = 2.33 mm (M1); λ = ax/D = 6.31 × 10⁻⁷ m → 6.3 × 10⁻⁷ m (A1, 2 s.f. consistent with data).
  2. (b) 12%
    % uncertainties add (M1): 7.1% + 0.54% + 4.0% = 12% (A1).
  3. (c) (630 ± 70) nm
    12% of 631 nm ≈ 70 nm (A1).
  4. (d) Measure across more fringes (or increase D) so that w is larger.
    B1: the 7% from w is largest; measure over more fringe spacings / use a larger D / use a travelling microscope or vernier calipers.
Q20Interference & coherence (two-source / double slit) · Challenge · Paper 2 style · 6 marks

Microwaves from a single transmitter pass through two gaps in a metal screen. The centres of the gaps are 12.0 cm apart. A detector moved along a line parallel to the screen and 1.20 m from it finds the central maximum and then the first-order maximum 0.30 m to one side of it.

  1. (a) Calculate the angle between the central line and the direction of the first-order maximum. [1]
  2. (b) Use the condition for a maximum to calculate the wavelength of the microwaves. [2]
  3. (c) Calculate the frequency of the microwaves. [1]
  4. (d) A student uses x = λD/a instead. Calculate the wavelength this gives and explain why it is not reliable here. [2]
Show answer
  1. (a) 14.0°
    tan θ = 0.30/1.20 → θ = 14.0° (A1).
  2. (b) 2.91 cm
    Path difference a sin θ = λ (M1): λ = 0.12 × sin 14.0° = 0.0291 m (A1).
  3. (c) 1.03 × 10¹⁰ Hz
    f = c/λ = 1.03 × 10¹⁰ Hz (A1).
  4. (d) 3.00 cm; the formula assumes small angles (x ≪ D), but here the angle is about 14°.
    λ = 0.30 × 0.12/1.20 = 0.0300 m (A1); B1: small-angle approximation (sin θ ≈ tan θ) not valid / slit separation not ≪ D.
Q21Interference & coherence (two-source / double slit) · Challenge · Paper 2 style · 6 marks

In a double-slit experiment the light waves from the two slits arrive at the screen with equal amplitude A, giving bright fringes and completely dark fringes. A filter is then placed over one slit so that the amplitude of the waves from that slit, at the screen, is halved.

  1. (a) Describe and explain the change in the appearance of the bright and dark fringes. [3]
  2. (b) Intensity is proportional to the square of the amplitude. Calculate the ratio of the intensity at a bright fringe to the intensity at a dark fringe after the change. [2]
  3. (c) Calculate the intensity at a bright fringe after the change as a fraction of the intensity at a bright fringe before the change. [1]
Show answer
  1. (a) Bright fringes become less bright; dark fringes are no longer completely dark; the fringe positions and spacing do not change.
    B1: resultant amplitude at a maximum falls from 2A to 1.5A → less bright; B1: at a minimum the amplitude is A − 0.5A = 0.5A ≠ 0 → not dark; B1: spacing unchanged since λ, D, a unchanged.
  2. (b) 9
    I ∝ (1.5A)² = 2.25A² and (0.5A)² = 0.25A² (M1); ratio = 9 (A1).
  3. (c) 0.56 (= 9/16)
    (1.5)²/(2)² = 2.25/4 = 0.5625 ≈ 0.56 (A1).
Q22Diffraction grating · Core · Paper 2 style · 4 marks

Yellow light of wavelength 589 nm from a sodium lamp is incident normally on a diffraction grating with 300 lines per millimetre.

  1. (a) Calculate the spacing between adjacent lines of the grating. [1]
  2. (b) Calculate the angle of the first-order maximum. [2]
  3. (c) Calculate the angle of the second-order maximum. [1]
Show answer
  1. (a) 3.33 × 10⁻⁶ m
    d = 1/(300 × 10³) = 3.33 × 10⁻⁶ m (A1).
  2. (b) 10.2°
    d sin θ = nλ (M1); sin θ = 589 × 10⁻⁹/3.33 × 10⁻⁶ → θ = 10.2° (A1).
  3. (c) 20.7°
    sin θ = 2λ/d → θ = 20.7° (A1).
Q23Diffraction grating · Standard · Paper 2 style · 4 marks

Light of wavelength 600 nm is incident normally on a diffraction grating with 500 lines per millimetre.

  1. (a) Determine the highest order of maximum that can be observed. [2]
  2. (b) Calculate the angle of this highest-order maximum. [1]
  3. (c) State the total number of bright maxima seen, including the zero order. [1]
Show answer
  1. (a) 3
    d = 1/500 mm = 2.0 × 10⁻⁶ m (M1); n ≤ d/λ = 3.33, so highest order is 3 (A1).
  2. (b) 64.2°
    sin θ = 3 × 600 × 10⁻⁹/2.0 × 10⁻⁶ = 0.90 → θ = 64.2° (A1).
  3. (c) 7
    B1: orders 0, ±1, ±2, ±3 → 7.
Q24Diffraction grating · Standard · Paper 2 style · 5 marks

A laser beam is directed normally at a diffraction grating with 400 lines per millimetre. On a screen 1.50 m from the grating, parallel to it, the two first-order spots are 0.82 m apart.

  1. (a) Calculate the angle between the zero-order and first-order beams. [2]
  2. (b) Calculate the wavelength of the laser light. [2]
  3. (c) State the colour of the light, giving a reason. [1]
Show answer
  1. (a) 15.3°
    Each first-order spot is 0.41 m from the centre (M1); tan θ = 0.41/1.50 → θ = 15.3° (A1).
  2. (b) 659 nm
    d = 1/(400 × 10³) = 2.50 × 10⁻⁶ m (M1); λ = d sin θ = 6.59 × 10⁻⁷ m (A1).
  3. (c) Red
    B1: 659 nm lies in the red part of the visible spectrum (about 620–700 nm).
Q25Diffraction grating · Standard · Paper 2 style · 4 marks

A student shines a green laser pointer of wavelength 532 nm normally at a diffraction grating whose label is missing. She measures the angle between the zero-order beam and the first-order beam as 18.6°.

  1. (a) Calculate the number of lines per millimetre on the grating. [2]
  2. (b) Suggest two reasons why a diffraction grating gives a more accurate value of wavelength than a double slit. [2]
Show answer
  1. (a) 600 lines per mm
    d = λ/sin θ = 532 × 10⁻⁹/sin 18.6° = 1.67 × 10⁻⁶ m (M1); 1/d = 600 per mm (A1).
  2. (b) The maxima are much sharper and brighter; they are at large angles that can be measured accurately.
    B1 each for any two: sharper (narrower) maxima; brighter maxima (many slits); large angles so smaller % uncertainty; can use higher orders.
Q26Diffraction grating · Challenge · Paper 2 style · 7 marks

Light from a hydrogen discharge tube contains a red line of wavelength 656 nm and a blue-green line of wavelength 486 nm. It falls normally on a grating with 600 lines per millimetre.

  1. (a) Determine the highest order observed for each line. [2]
  2. (b) Calculate the angle between the two lines in the second-order spectrum. [3]
  3. (c) Explain why a grating with more lines per millimetre would separate the lines better, and state one disadvantage. [2]
Show answer
  1. (a) red: 2; blue-green: 3
    d = 1.67 × 10⁻⁶ m (M1); d/λ = 2.54 for red → 2; 3.43 for blue-green → 3 (A1).
  2. (b) 16.2°
    θ = sin⁻¹(2λ/d): red 51.9° (M1), blue-green 35.7° (M1); difference 16.2° (A1).
  3. (c) Smaller d gives larger angles, so a greater angular separation; but fewer orders are visible.
    B1: sin θ = nλ/d, so smaller d → larger angles and spread; B1: fewer orders observable (n_max = d/λ smaller).
Q27Diffraction grating · Challenge · Paper 1 style · 1 mark
  1. (a) Monochromatic light falls normally on a diffraction grating. The second-order maximum is at 30.0° to the straight-through direction. At what angle is the first-order maximum? [1]
Show answer
  1. (a) B 14.5°
    d sin θ = nλ: sin θ₁ = ½ sin 30° = 0.25, so θ₁ = 14.5°. 15.0° wrongly halves the angle instead of halving sin θ.
Q28Diffraction · Core · Paper 2 style · 3 marks
  1. (a) State what is meant by diffraction. [1]
  2. (b) Water waves of wavelength 1.5 cm pass through a gap in a barrier in a ripple tank. Describe how the pattern of waves beyond the gap changes as the gap width is reduced from 10 cm to 1.5 cm. [2]
Show answer
  1. (a) The spreading of a wave as it passes through a gap or around an edge.
    B1: spreading of waves through a gap/past an obstacle.
  2. (b) The waves spread out more (diffraction increases) as the gap becomes similar to the wavelength; the wavelength stays the same.
    B1: more spreading/curved wavefronts when gap ≈ λ; B1: wavelength (spacing of wavefronts) unchanged.
Q29Diffraction · Standard · Paper 1 style · 1 mark
  1. (a) [1]
Show answer
  1. (a) C The wavelength of sound is similar to the width of the doorway but the wavelength of light is much smaller.
    Diffraction is significant when the wavelength is comparable to the gap; audible sound has wavelengths of the order of a metre, light about 5 × 10⁻⁷ m. Wave type (A) and speed (B) do not decide the amount of diffraction.
Q30Diffraction · Challenge · Paper 2 style · 4 marks

A long-wave radio transmitter broadcasts at 198 kHz and an FM transmitter at 100 MHz. Speed of electromagnetic waves = 3.00 × 10⁸ m s⁻¹.

  1. (a) Calculate the wavelength of each radio signal. [2]
  2. (b) A village lies in a valley behind a range of hills about 1 km wide. Explain why the long-wave signal can be received in the village but the FM signal cannot. [2]
Show answer
  1. (a) 1520 m and 3.0 m
    λ = c/f: 3.00 × 10⁸/198 × 10³ = 1520 m (A1); 3.00 × 10⁸/100 × 10⁶ = 3.0 m (A1).
  2. (b) The long-wave wavelength is comparable to the size of the hills, so it diffracts significantly around/over them; the FM wavelength is much smaller, so it hardly diffracts and the village is in its 'shadow'.
    B1: diffraction significant when λ comparable to obstacle size (≈ 1.5 km vs 1 km); B1: 3 m ≪ 1 km, so little diffraction → shadow region.

Similar questions

Questions that test the same subtopic in different years, grouped so you can work on one skill at a time.

References only: find each question in its paper (official link where available, otherwise through your school).

Superposition principle & stationary waves Banker62 questions · 9/9 sessions
Interference & coherence (two-source / double slit) Banker41 questions · 9/9 sessions
Diffraction grating Banker33 questions · 9/9 sessions
Diffraction Banker28 questions · 9/9 sessions

Subtopics

Our analysis of how often each subtopic was examined and how many marks it carried, 2022 to May/June 2026.

SubtopicMarks indexedSessions
Superposition principle & stationary waves Banker1249/9
Interference & coherence (two-source / double slit) Banker1079/9
Diffraction grating Banker619/9
Diffraction Banker329/9

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