8.1.3Waves and superposition
Wavelength of Stationary Waves
5 min read 8 parts Lesson 14 of 21 1 quiz
Lesson summary
8.1.3 Wavelength of Stationary Waves — AS PHYSICS 9702 notes: Find the wavelengths and frequencies of harmonics on strings and in air columns.Frequency — stationary waves have different patterns depending on the frequency of vibration.Situation — the pattern also depends on how t…
- Resonant frequencies
- Fundamental mode
- Higher harmonics
- nth harmonic
- Higher modes
- Harmonics present
Section 1 of 8Patterns depend on the situation
Frequency
- Frequency stationary waves have different patterns depending on the frequency of vibration.
Situation
- Situation the pattern also depends on how the wave is created, such as a string or an air column.
Resonant frequencies
- Resonant frequencies the possible frequencies depend on the length L and the wave speed v.
Section 2 of 8String fixed at both ends
Fundamental mode
- Fundamental mode the simplest pattern is a single loop of two nodes and one antinode, also called the first harmonic.
Wavelength
- Wavelength only half a wavelength fits in the string, so λ1 = 2L.
Higher harmonics
- Higher harmonics they appear as the frequency increases.
nth harmonic
- nth harmonic it has n antinodes and n + 1 nodes, with wavelength λn = 2L/n.
- The second harmonic has three nodes and two antinodes, with λ = L.
- The third harmonic has four nodes and three antinodes, with λ = 2L/3.
Frequency
- Frequency found from the wave equation, fn = v/λn = nv/2L.
Section 3 of 8Air column closed at one end
Ends
- Ends a node forms at the closed end and an antinode at the open end.
Fundamental
- Fundamental a quarter wavelength with one node and one antinode, so L = λ/4.
Higher modes
- Higher modes each extra harmonic adds one node and one antinode.
Harmonics present
- Harmonics present only odd harmonics form.
General length
- L = nλ/4 with n odd, for example L = 3λ/4 for the third harmonic.
Section 4 of 8Air column open at both ends
Ends
- Ends an antinode forms at each open end.
Fundamental
- Fundamental half a wavelength with one node and two antinodes, so L = λ/2.
Higher modes
- Higher modes each extra harmonic adds one node and one antinode.
Harmonics present
- Harmonics present odd and even harmonics both form.
General length
- L = nλ/2.
Section 5 of 8Harmonic numbering
Harmonic numbering
Fundamental
- Fundamental it is the first harmonic, n = 1, the lowest frequency.
Both ends fixed or both open
- Both ends fixed or both open a full wavelength is the second harmonic.
Matching
- Matching match the wavelength to the harmonic named in the question, for example the second lowest note in a closed pipe is the third harmonic.
Section 6 of 8More from the specification
1Reflected ultrasonic wave pulses
- Reflected ultrasonic wave pulses transmitting periodic wave pulses along boundaries creates interfering counter-propagating waves forming stable stationary harmonics.
2Displacement
- Change in position.
3Amplitude
- Maximum displacement from equilibrium.
4Resultant
- Vector sum of two or more vectors.
5Pulse
- Single disturbance travelling through a medium.
6Loudspeaker
- Device that converts an electrical signal into sound by the motor effect.
7Standing wave
- A pattern formed by two identical waves travelling in opposite directions, with fixed nodes and antinodes.
8Origin
- Origin a stationary wave arises from superposition of a wave and its reflection;
- adjacent nodes, or adjacent antinodes, are half a wavelength apart.
Section 7 of 8Key terms
| Term | Meaning |
|---|---|
| Fundamental mode | Simplest stationary wave pattern with the lowest resonant frequency, the first harmonic. |
| Harmonic | Resonant mode of a stationary wave, with frequency a whole-number multiple of the fundamental where allowed. |
| Resonant frequency | Frequency at which a stationary wave forms in a string or air column. |
| Closed pipe | Pipe closed at one end with a node there and an antinode at the open end. |
| Open pipe | Pipe open at both ends with an antinode at each end. |
Section 8 of 8Exam technique
1
Using L = λ for the fundamental of a string — the fundamental has L = λ/2.
2
Allowing even harmonics in a pipe closed at one end — only odd harmonics occur.
3
Putting an antinode at a closed end — a closed end is a node.
4
Naming the second lowest note in a closed pipe the second harmonic — it is the third harmonic.