Playbook
Waves
The wave equation, strings and pipes, beats and the Doppler effect. Half its questions have numeric answers.
- Questions in the bank
- 80
- q/paper in 2025–26
- 0.55
- Numeric answer
- 50%
- Notes pages
- 5
Tier: Long tail
When you’ll see it
A wave equation in x and t, a string or pipe at resonance, the speed of sound or of a wave on a string, beats, or a moving source or listener.
How this chapter is tested
Waves sits in the long tail, and many of its questions ask for a number. Most are short: read ω and k off an equation, pick the right harmonic formula, or write one Doppler ratio, and the answer follows in two or three lines.
The work is in the bookkeeping. Expand any common factor before reading ω and k, and keep k in m⁻¹ when the speed is asked in m/s. On strings and pipes, keep harmonics and overtones apart: a closed pipe has only odd harmonics, so its first overtone is the third harmonic. Speeds need T in kelvin and μ in kilograms per metre.
The Doppler page rewards a rule over a memorised sign pattern: motion towards raises the frequency, and an echo from a wall is shifted twice. The sine equation is the one from Oscillations, and superposition returns in Wave Optics.
The sub-skills
The distinct skills inside the chapter, in the order to learn them.
The wave equation
In y = A sin(ωt − kx), f = ω/2π, λ = 2π/k and v = ω/k; same signs on t and x mean travel along −x; the largest particle speed is Aω.
Wave speed
√(T/μ) on a string, √(Y/ρ) in a rod, √(γRT/M) in a gas; at a fixed temperature, pressure alone does not change the speed of sound.
Superposition and strings
Resultant amplitude by the cosine rule; a string fixed at both ends has every harmonic nv/2L, and its frequency goes as √T.
Organ pipes and the resonance tube
Open pipe nv/2L, closed pipe only (2n − 1)v/4L; the end correction is 0.3d, and v = 2f(l₂ − l₁) needs no end correction.
Beats and the Doppler effect
Beat frequency |f₁ − f₂|; heard frequency f(v ± vₒ)/(v ∓ vₛ), with each sign set so that approach raises it; an echo is shifted twice.
Traps to expect
Distractor shapes this chapter reuses. The Traps page covers the ones that cut across chapters.
k left in cm⁻¹
When x is in cm, ω/k comes out in cm/s, a hundred times larger than the value in m/s. Convert k to m⁻¹ first.
Overtone read as harmonic
The first overtone of a closed pipe is the third harmonic, because the second harmonic does not exist there.
Beats in a time
Ten beats in two seconds is a beat frequency of five hertz, not ten. Divide by the time before using the difference.
An echo shifted once
A driver moving towards a wall hears the echo at f(v + u)/(v − u). Applying the formula once, for the source only, misses the second shift.
Learn it before you drill it
This chapter has full teaching notes — foundations, worked examples, self-checks and a mastery check for each page. Read the notes once, then drill page by page below.
Waves notesDrill every Waves question
80 questions from the bank, across 5 subtopics.
Drill one subtopic at a time
The 5 subtopics, in teaching order.
- Wave Equation and Particle MotionDrill Wave Equation and Particle Motion
- Wave Speed in Strings, Solids and GasesDrill Wave Speed in Strings, Solids and Gases
- Superposition and Standing Waves on StringsDrill Superposition and Standing Waves on Strings
- Organ Pipes and the Resonance TubeDrill Organ Pipes and the Resonance Tube
- Beats and the Doppler EffectDrill Beats and the Doppler Effect
Related playbooks
Often paired with this one — the technique or the trap overlaps. Drill these next.