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IB Physics Standing Waves: Concept & Exam Guide
Answered by RevisionPrep's IB Educators
Standing waves trip up more IB Physics students than almost any other topic in Waves, mostly because the maths looks easy but the reasoning gets tested hard. Here's what actually comes up, and how to answer it properly.
The Core Concept
What is standing waves in IB Physics, and how is it examined?
A standing (stationary) wave forms when two identical waves travelling in opposite directions superpose — usually an incident wave and its reflection. Unlike a travelling wave, it doesn't transfer energy along its length; it has fixed nodes (zero displacement) and antinodes (maximum displacement). It's examined in Topic 4 (SL & HL) via diagrams, harmonic calculations and short-answer or data-based questions.
According to the IB Physics guide (first assessment 2025), standing waves sit under Topic 4.3 (Wave phenomena, HL extension) alongside diffraction and the Doppler effect, though the basic formation mechanism is introduced at SL in Topic 4.1. Expect it paired with resonance and pipes/strings problems in Paper 1 and Paper 2.
What's the difference between a standing wave and a travelling wave?
A travelling wave carries energy from one point to another and every particle along it has the same amplitude, just a phase delay. A standing wave stores energy locally — particles between adjacent nodes oscillate in phase but with different amplitudes, and no net energy moves past a node. That's the one-sentence answer examiners want on a 'compare' question.
Quick tip: if a question asks you to distinguish the two, always mention energy transfer explicitly — students who describe only the shape (not the energy) tend to lose the second marking point.
What are nodes and antinodes?
A node is a point on a standing wave with zero displacement at all times — the wave's amplitude is always zero there. An antinode is a point of maximum displacement, oscillating with the largest amplitude in the pattern. Adjacent nodes are always separated by half a wavelength, and an antinode sits exactly midway between them.
Common mistake: students confuse 'node' with 'zero velocity'. Actually, particles at an antinode have zero velocity only at maximum displacement — it's the node that has zero displacement at every instant, not zero velocity everywhere.
Harmonics, Strings & Pipes
How do you calculate the frequencies of harmonics on a string?
For a string fixed at both ends, the nth harmonic frequency is , where is wave speed, is string length, and . The fundamental () has one antinode and two nodes; each higher harmonic adds one more node and antinode.
Worked example: A 0.60 m guitar string has wave speed 320 m/s. Fundamental: . Third harmonic: . Note IB questions often give you tension and mass per unit length instead of directly, so you'll need first.
How is a standing wave different in a pipe open at both ends versus closed at one end?
An open-open pipe has an antinode at each open end and supports all harmonics: . A closed-open pipe has a node at the closed end and an antinode at the open end, supporting only odd harmonics: for . Mixing these two formulas up is the single most common exam error on this topic.
| Pipe type | End conditions | Harmonics allowed | Fundamental formula |
|---|---|---|---|
| Open-open | Antinode-antinode | All (n=1,2,3…) | f = v/2L |
| Closed-open | Node-antinode | Odd only (n=1,3,5…) | f = v/4L |
Quick tip: sketch the actual displacement pattern before you touch a formula — examiners award marks for correctly placed nodes/antinodes even if the arithmetic slips.
Why does a closed pipe only produce odd harmonics?
Because the closed end must always be a node and the open end must always be an antinode, only wave patterns that fit a node at one end and antinode at the other are physically possible. That geometric constraint only allows odd multiples of the quarter-wavelength pattern — the even harmonics simply don't satisfy both boundary conditions simultaneously.
Try sketching for a closed pipe: you'd need a node at both ends, which contradicts the open end needing an antinode. That's why it's excluded — it's a boundary condition problem, not an energy one.
Exam Technique & Common Mistakes
What mistakes do students make with standing waves in exams?
The three recurring errors I see every year marking mocks: mixing up the open-pipe and closed-pipe harmonic formulas, forgetting that wavelength (not distance between nodes) equals twice the node-to-node spacing when reading off diagrams, and describing standing waves as 'transferring no energy at all' instead of 'no net energy transfer past a node'.
- Always label explicitly before substituting into a harmonic formula.
- Double-check whether the pipe/string diagram shows the fundamental or a higher harmonic — count antinodes, not nodes, to find .
- When asked to 'explain' formation, mention superposition, reflection, and phase — a bare formula gets you no marks on an explain question.
How are standing waves assessed on Paper 1 and Paper 2?
Paper 1 (multiple choice) usually tests quick harmonic-number or wavelength identification from a diagram. Paper 2 typically gives a longer structured question: derive a frequency, explain formation using superposition, or link resonance to a real-world scenario like a wine glass or bridge. HL papers sometimes extend into diffraction gratings or the Doppler effect within the same question.
According to the IB Physics guide, Paper 2 command terms here are usually 'calculate', 'determine', 'explain' or 'sketch' — 'explain' questions specifically want you to reference superposition and reflected waves, not just describe the pattern.
What formulas do I actually need to memorise for standing waves?
You need for strings and open-open pipes, (odd n only) for closed-open pipes, and for wave speed on a string. The IB Physics data booklet gives most wave equations, but not always the harmonic-number relationships — you're expected to derive those from the boundary conditions on the spot.
Quick tip: the data booklet won't hand you 'only odd harmonics for closed pipes' as a written rule — that reasoning has to come from you, so practise sketching the first three harmonics for each pipe type until it's automatic.
SL vs HL & Related Topics
Is standing waves the same for SL and HL Physics?
The core concept — nodes, antinodes, harmonic formulas for strings and pipes — is shared by SL and HL students. HL students go further, connecting standing waves to diffraction gratings, resonance in more complex systems, and sometimes multi-step problems combining wave phenomena with the Doppler effect in the same question.
| Aspect | SL | HL |
|---|---|---|
| Node/antinode basics | Yes | Yes |
| Harmonic formulas (string & pipe) | Yes | Yes |
| Combined with diffraction/Doppler | Rare | Common |
| Multi-step Paper 2 questions | Shorter | Longer, multi-part |
How does resonance relate to standing waves?
Resonance happens when a system is driven at one of its natural (harmonic) frequencies, causing a standing wave pattern to build up with large, stable amplitude. A guitar string resonates at its fundamental and harmonics; an organ pipe resonates at the frequencies allowed by its boundary conditions. Standing waves are essentially what resonance looks like once it's established.
Examiners like to link this to real examples — the Tacoma Narrows Bridge or a wine glass shattering are classic IB-style contexts for explaining resonance driving a standing wave to destructive amplitude.
Should my child worry if they're struggling with standing waves — is it a big part of the final grade?
Standing waves is one sub-topic within the broader Waves topic, so it won't sink an overall grade on its own — but it recurs across Paper 1 and Paper 2, and often reappears combined with resonance or the Doppler effect in the same question. Getting the boundary-condition logic solid early pays off across several exam questions, not just one.
It's worth having your child work through past-paper Waves questions specifically rather than just re-reading notes — this topic rewards pattern recognition (spotting which pipe/string case you're in) more than memorisation.
Standing Wave Formulas: String & Pipe Cases
| Setup | Boundary conditions | Harmonics allowed | Fundamental frequency |
| String (fixed both ends) | Node-node | All (n=1,2,3…) | f = nv/2L |
| Open-open pipe | Antinode-antinode | All (n=1,2,3…) | f = nv/2L |
| Closed-open pipe | Node-antinode | Odd only (n=1,3,5…) | f = nv/4L |
For worked past-paper questions, harmonic-diagram drills and full Waves topic notes, check the Physics Revision Notes and Topical Worksheets on revisionprep.com.
