IB PHYSICS • WAVE BEHAVIOUR

Understand Standing Waves & Resonance — Understand C.4 Standing waves and resonance

Discover how confined waves create fixed patterns of vibration that shape music, engineering, and physics.

Historical Context & Motivation

For centuries, musicians have known that a plucked string or a blown pipe produces certain musical notes and not others. The question of why only specific frequencies ring out—while most disturbances die away—puzzled natural philosophers long before the physics of waves was formalized. The answer lies in standing waves and resonance, phenomena that arise whenever waves are confined to a bounded region.

~500 BCE
Pythagoras & Musical Harmony
Pythagoras discovered that strings whose lengths form simple ratios (2:1, 3:2) produce harmonious intervals—an early observation of standing wave patterns on strings.
1638
Mersenne's Laws
Marin Mersenne published mathematical relationships linking a vibrating string's frequency to its length, tension, and linear mass density.
1787
Chladni Figures
Ernst Chladni sprinkled sand on vibrating plates and revealed intricate two-dimensional standing wave patterns, captivating audiences including Napoleon.
1842
Doppler & Wave Theory Advances
Christian Doppler's work on wave frequency shifts reinforced the broader wave framework that underpins the study of resonance.
1940
Tacoma Narrows Bridge Collapse
The dramatic collapse of this suspension bridge became the most famous real-world illustration of resonance, showing engineers that standing wave modes can have catastrophic consequences.

The central question this topic addresses is: when two waves of the same frequency travel in opposite directions through the same medium, what pattern forms, and why does the medium prefer only certain frequencies? Understanding this will connect your knowledge of travelling waves to applications in music, telecommunications, and even quantum mechanics.

Core Principles & Definitions

A standing wave (also called a stationary wave) is the result of two identical travelling waves moving in opposite directions through the same medium. Unlike a travelling wave, which transports energy continuously from one place to another, a standing wave stores energy in a fixed spatial pattern. The wave appears to vibrate in place: certain points remain permanently at rest while others oscillate with maximum amplitude.

1

Superposition

When two or more waves overlap, the resultant displacement at any point is the algebraic sum of the individual displacements. This principle of superposition is the foundation of standing waves.
2

Nodes & Antinodes

Nodes are points of permanent zero displacement where destructive interference always occurs. Antinodes are points of maximum displacement where constructive interference is greatest. Nodes and antinodes alternate at equal spacing of λ/2.
3

Boundary Conditions

The ends of the medium (fixed or free) determine which standing wave patterns are allowed. A fixed end must be a node; a free (open) end must be an antinode.
4

Harmonics

Only specific frequencies produce stable standing waves. These are called harmonics. The lowest allowed frequency is the fundamental (1st harmonic); higher harmonics are integer multiples of it.
5

Resonance

Resonance occurs when an external driving frequency matches one of the system's natural frequencies. At resonance, energy transfer is maximized and the amplitude of the standing wave grows dramatically.
KEY TAKEAWAY
Think of a standing wave like pushing a child on a swing. If you push at random times, the swing barely moves. But if you push at exactly the right moment each cycle—matching the swing's natural frequency—the amplitude builds dramatically. That's resonance. Standing waves are the spatial patterns that form when a system resonates.

Visual Explanation — Formation of Standing Waves

The diagram below shows how two travelling waves—one moving to the right (blue) and one moving to the left (violet)—superpose to create a standing wave (cyan). Notice that the nodes remain stationary while the antinodes oscillate between maximum positive and maximum negative displacement.

Two identical travelling waves (blue and violet) move in opposite directions. Their superposition produces a standing wave (cyan). Pink dots mark nodes (N) and gold dots mark antinodes (A). The dashed cyan curve shows the wave at a different instant, illustrating that it oscillates in place.

Several key observations emerge from this diagram. First, the distance between two adjacent nodes (or two adjacent antinodes) is exactly half a wavelength (λ/2). Second, all points between two consecutive nodes vibrate in phase with each other, while points on opposite sides of a node are in antiphase (180° out of phase). Third, no energy is transported past a node—energy remains trapped between nodes, oscillating between kinetic and potential forms.

Mathematical Framework

The mathematical description of standing waves builds directly on the wave equation. When two travelling waves with the same amplitude, frequency, and wavelength move in opposite directions, their superposition yields a standing wave whose displacement depends on position and time separately.

SUPERPOSITION OF TWO TRAVELLING WAVES
y(x, t) = 2A sin(2πx / λ) × cos(2πft)
Where A = amplitude of each travelling wave, λ = wavelength, f = frequency, x = position along the medium, t = time. The term sin(2πx/λ) determines the spatial pattern; cos(2πft) determines temporal oscillation.

Notice how position (x) and time (t) are in separate trigonometric functions. This is fundamentally different from a travelling wave, where they appear together as sin(kx − ωt). The separation means the wave shape doesn't move—it simply oscillates in amplitude over time.

HARMONIC FREQUENCIES — STRINGS (BOTH ENDS FIXED)
fₙ = n × v / (2L) where n = 1, 2, 3, …
fₙ = frequency of the nth harmonic, v = wave speed on the string, L = length of the string, n = harmonic number (positive integer). The fundamental frequency is f₁ = v/(2L).
HARMONIC FREQUENCIES — OPEN PIPE (BOTH ENDS OPEN)
fₙ = n × v / (2L) where n = 1, 2, 3, …
Open pipes have antinodes at both ends and behave identically to a string fixed at both ends in terms of allowed harmonics—all integer harmonics are present.
HARMONIC FREQUENCIES — CLOSED PIPE (ONE END CLOSED)
fₙ = n × v / (4L) where n = 1, 3, 5, … (odd integers only)
A closed pipe has a node at the closed end and an antinode at the open end. Only odd harmonics are allowed, giving this type of pipe a distinctly different timbre from an open pipe.
💡 IB Exam Tip
Always check the boundary conditions first. Ask yourself: is each end a node or an antinode? This determines whether you use the string/open-pipe formula (n × v / 2L, all harmonics) or the closed-pipe formula (n × v / 4L, odd harmonics only).

Harmonics on Strings & in Pipes

The pattern of harmonics depends entirely on the boundary conditions of the vibrating system. The diagram below illustrates the first three harmonics for a string fixed at both ends, an open pipe, and a pipe closed at one end. Pay close attention to the positions of nodes (N) and antinodes (A) at the boundaries.

Comparison of the first three allowed harmonics for a string fixed at both ends (left), an open pipe (center), and a pipe closed at one end (right). Notice that the closed pipe supports only odd harmonics (n = 1, 3, 5, …), which gives it a distinctive hollow sound.
Summary of standing wave systems and their allowed harmonics
SystemBoundary ConditionsAllowed HarmonicsFundamental Wavelength
String (fixed–fixed)Node at both endsAll integers: n = 1, 2, 3, …λ₁ = 2L
Open pipe (open–open)Antinode at both endsAll integers: n = 1, 2, 3, …λ₁ = 2L
Closed pipe (closed–open)Node at closed, antinode at openOdd integers only: n = 1, 3, 5, …λ₁ = 4L

Worked Example — Guitar String Harmonics

A guitar string has a length of 0.65 m and is fixed at both ends. When plucked, the fundamental frequency is 330 Hz. Determine (a) the wave speed on the string, (b) the frequency and wavelength of the 3rd harmonic, and (c) the number of nodes and antinodes in the 3rd harmonic.

Guitar String — 3rd Harmonic
1
Step 1 — Identify Given ValuesLength of string: L = 0.65 m. Fundamental frequency: f₁ = 330 Hz. Both ends are fixed, so the system supports all integer harmonics (n = 1, 2, 3, …).
2
Step 2 — Find the Wave SpeedFor a string fixed at both ends, the fundamental satisfies f₁ = v/(2L). Rearranging: v = f₁ × 2L = 330 Hz × 2 × 0.65 m.
v = 429 m s⁻¹
3
Step 3 — Find the 3rd Harmonic FrequencyThe nth harmonic frequency is fₙ = n × f₁. For n = 3: f₃ = 3 × 330 Hz.
f₃ = 990 Hz
4
Step 4 — Find the 3rd Harmonic WavelengthUsing v = fλ → λ₃ = v/f₃ = 429/990 ≈ 0.433 m. Alternatively, L = 3λ₃/2 → λ₃ = 2L/3 = 2(0.65)/3 ≈ 0.433 m. Both methods agree.
λ₃ ≈ 0.433 m
5
Step 5 — Count Nodes and AntinodesFor the nth harmonic on a fixed–fixed string, there are (n + 1) nodes and n antinodes. For n = 3: nodes = 4, antinodes = 3. The nodes include the two endpoints plus two interior nodes.
4 nodes, 3 antinodes

Travelling Waves vs Standing Waves

It is essential for IB Physics that you can clearly distinguish between travelling waves and standing waves. Although both involve oscillation, their properties differ in several fundamental ways. The table below highlights these differences side by side.

Key differences between travelling and standing waves
PropertyTravelling WaveStanding Wave
Energy TransferTransfers energy in the direction of propagationNo net energy transfer; energy is stored between nodes
AmplitudeAll points oscillate with the same amplitudeAmplitude varies from zero (node) to maximum (antinode)
PhasePhase changes continuously along the direction of travelAll points between adjacent nodes are in phase; across a node they are in antiphase
FrequencyAny frequency is possibleOnly specific (resonant) frequencies are sustained
Wave PatternProfile moves through spaceProfile oscillates in place
Wavelength MeasurementDistance between identical points in phase (e.g., crest to crest)Twice the distance between adjacent nodes (or adjacent antinodes)
KEY TAKEAWAY
Imagine a travelling wave as water flowing through a hose—energy moves from one end to the other. A standing wave is more like water sloshing back and forth in a bathtub—energy stays trapped inside the system, alternating between kinetic and potential forms, but it never leaves the tub. The nodes act as walls that confine the energy.

Connections to Advanced Topics

Standing waves are not limited to strings and pipes. The same physics appears in a remarkable range of contexts, from the microscopic to the cosmic. At the university level, the concept of quantized standing wave patterns becomes the foundation for understanding matter itself.

How IB standing wave concepts extend to advanced physics
IB-Level ConceptAdvanced Extension
Standing waves on a string with quantized frequenciesElectron standing waves in atoms (de Broglie model): only specific wavelengths fit around the orbit, explaining quantized energy levels
Resonance at natural frequencies of a systemResonance in electrical circuits (RLC circuits): current peaks when driving frequency matches the circuit's natural frequency ω₀ = 1/√(LC)
Harmonics in pipes (1D standing waves)2D and 3D standing waves: Chladni patterns on plates, seismic modes of the Earth, and microwave cavity modes
Nodes and antinodes in mechanical wavesNodes in electromagnetic standing waves: used in laser cavities and microwave ovens to create stable oscillation patterns

Perhaps the most profound connection is to quantum mechanics. In the early twentieth century, Louis de Broglie proposed that electrons behave as waves. The requirement that electron standing waves form complete loops around an atomic nucleus leads directly to Bohr's quantized energy levels. In this view, atoms are like tiny three-dimensional resonant cavities, and chemistry is essentially the physics of standing waves.

Practice Problems

PROBLEM 1CONCEPTUAL
A standing wave is established on a string fixed at both ends. Explain why energy is not transferred along the string, even though the string is clearly vibrating. In your answer, refer to nodes and the phase relationship of points on either side of a node.
PROBLEM 2BASIC CALCULATION
A string of length 1.2 m is fixed at both ends. The speed of transverse waves on the string is 180 m s⁻¹. Calculate (a) the fundamental frequency and (b) the wavelength of the 4th harmonic.
PROBLEM 3INTERMEDIATE
An organ pipe open at both ends has a fundamental frequency of 262 Hz (middle C). The speed of sound in the pipe is 343 m s⁻¹. (a) Calculate the length of the pipe. (b) If one end of the pipe is now closed, determine the new fundamental frequency and state which harmonics are present.
PROBLEM 4APPLIED
A microwave oven operates at a frequency of 2.45 GHz. Microwaves form standing waves inside the oven cavity, and food items placed at antinodes heat faster than those at nodes. The speed of microwaves is 3.00 × 10⁸ m s⁻¹. (a) Calculate the wavelength of the microwaves. (b) Determine the distance between adjacent nodes inside the oven. (c) Explain why microwave ovens use a rotating turntable.
PROBLEM 5CRITICAL THINKING
A student claims that a pipe which is open at one end and closed at the other can never produce the same frequency as a pipe of the same length that is open at both ends. Using the harmonic frequency formulas, evaluate this claim. Is the student correct? Provide a mathematical argument.

Lesson Summary

Standing waves form when two identical travelling waves move in opposite directions through the same medium, creating a pattern of fixed nodes (zero displacement) and antinodes (maximum displacement). The boundary conditions—whether each end is fixed (node) or free (antinode)—determine which harmonics are allowed. A string fixed at both ends and an open pipe support all integer harmonics with fₙ = nv/(2L), while a pipe closed at one end supports only odd harmonics with fₙ = nv/(4L).

Resonance occurs when a system is driven at one of its natural frequencies, causing the amplitude to build dramatically because energy is transferred efficiently into the system. Unlike travelling waves, standing waves do not transport energy—they store it between nodes. The distance between adjacent nodes (or adjacent antinodes) equals half a wavelength (λ/2). These principles connect to applications ranging from musical instruments and microwave ovens to the quantized energy levels of atoms in quantum mechanics.

Varsity Tutors • IB Physics • Understand Standing Waves & Resonance