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October 18, 2026

Oscillations and waves

ZIMSEC A Level · Physics · Form 5, Form 6

Simple harmonic motion

Acceleration is proportional to displacement and directed towards the equilibrium position: a = −ω²x.

  • x = x₀ sin ωt; v = ±ω√(x₀² − x²); maximum speed ω x₀; maximum acceleration ω² x₀.
  • Pendulum: T = 2π√(l/g); mass–spring: T = 2π√(m/k).
  • Damping reduces amplitude; resonance occurs when the driving frequency equals the natural frequency.

Worked example: A simple pendulum has a length of 0.80 m. Find its period (g = 9.81 m s⁻²).

T = 2π√(0.80/9.81) = 2π × 0.2856 = 1.79 s

Waves

  • v = fλ. Intensity ∝ amplitude². Transverse waves can be polarised; longitudinal waves cannot.
  • Doppler effect for sound: observed frequency f′ = fv/(v ± vs) (minus when the source approaches).

Superposition

  • Stationary waves form from two waves travelling in opposite directions: nodes (zero amplitude) and antinodes; distance between nodes = λ/2.
  • Diffraction is greatest when the gap is similar to the wavelength.
  • Two-source interference: fringe spacing x = λD/a.
  • Diffraction grating: d sin θ = nλ.

Worked example: Light of wavelength 600 nm falls on a grating with 300 lines per mm. Find the angle of the first-order maximum.

d = 1/300 000 m = 3.33 × 10⁻⁶ m; sin θ = 600 × 10⁻⁹ ÷ 3.33 × 10⁻⁶ = 0.180 → θ = 10.4°

Exam tip: Convert lines per mm into slit spacing d in metres before using d sin θ = nλ.

Check yourself

  1. A wave has frequency 50 Hz and wavelength 6.8 m. Find its speed.
  2. What is the distance between adjacent nodes in a stationary wave?
  3. State the condition for resonance.
Show answers
  1. 340 m s⁻¹
  2. Half a wavelength (λ/2).
  3. The driving frequency equals the natural frequency of the system.

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