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How do we describe a wave and what does it transfer?

Transverse and longitudinal waves, amplitude, wavelength, frequency, period and speed, the wave equation, phase and phase difference, and polarisation of transverse waves.

A focused answer to the Edexcel 9PH0 wave basics content, covering transverse and longitudinal waves, amplitude, wavelength, frequency, period and speed, the wave equation, phase and phase difference, and polarisation.

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What this dot point is asking

Edexcel wants you to distinguish transverse and longitudinal waves, define amplitude, wavelength, frequency, period and speed, apply the wave equation v=fλv = f\lambda, work with phase and phase difference, and explain polarisation of transverse waves.

The answer

Transverse and longitudinal waves

Light and other electromagnetic waves, and waves on a string, are transverse. Sound and seismic P-waves are longitudinal. In both, individual particles oscillate about a fixed point while the energy travels onward.

Describing a wave

The amplitude of a wave determines its intensity: intensity is proportional to the square of the amplitude. Frequency is set by the source and does not change when the wave moves into a new medium, even though the speed and wavelength do.

The wave equation

This single equation links the three core wave quantities and is used constantly. It follows directly from the definition of speed: in one period the wave moves forward one wavelength.

Phase and phase difference

Phase describes the stage a point has reached in its cycle. Two points exactly one wavelength apart are in phase (phase difference of 360360 degrees or 2π2\pi radians); half a wavelength apart they are in antiphase (180180 degrees or π\pi radians). Phase difference can be found from path difference: a path difference of λ\lambda corresponds to a phase difference of 2π2\pi.

Polarisation

Passing unpolarised light through one filter polarises it; a second filter (analyser) at 9090 degrees to the first blocks it entirely. This is direct evidence that light is a transverse wave, since sound (longitudinal) cannot be polarised.

Examples in context

Polaroid sunglasses cut glare by blocking the horizontally polarised light reflected from roads and water. The wave equation underpins all of acoustics and optics, from tuning instruments to designing antennas. Seismologists distinguish longitudinal P-waves from transverse S-waves to locate earthquakes and probe the Earth's interior (S-waves cannot pass through the liquid outer core). Phase difference is central to interference, sonar, and the way stereo sound is recorded and reproduced.

Try this

Q1. State the wave equation. [1 mark]

  • Cue. v=fλv = f\lambda, wave speed equals frequency times wavelength.

Q2. A radio wave has frequency 1.0×1081.0 \times 10^{8} Hz and travels at 3.0×1083.0 \times 10^{8} m per second. Find its wavelength. [2 marks]

  • Cue. λ=vf=3.0×1081.0×108=3.0\lambda = \frac{v}{f} = \frac{3.0 \times 10^{8}}{1.0 \times 10^{8}} = 3.0 m.

Q3. Explain why sound cannot be polarised. [2 marks]

  • Cue. Sound is longitudinal, oscillating along the direction of travel, so there is no perpendicular plane of oscillation to restrict.

Exam-style practice questions

Practice questions written in the style of Pearson Edexcel exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Edexcel 20173 marksA sound wave has a frequency of 256256 Hz and travels at 340340 m per second. Calculate its wavelength.
Show worked answer →

Wave equation: v=fλv = f\lambda, so λ=vf\lambda = \frac{v}{f}.

λ=340256=1.3\lambda = \frac{340}{256} = 1.3 m.

Markers reward v=fλv = f\lambda, the correct rearrangement, and the value about 1.31.3 m.

Edexcel 20204 marksDescribe the difference between transverse and longitudinal waves, giving one example of each, and explain why only transverse waves can be polarised.
Show worked answer →

In a transverse wave the oscillations are perpendicular to the direction of energy transfer (for example, light or a wave on a string). In a longitudinal wave the oscillations are parallel to the direction of energy transfer, producing compressions and rarefactions (for example, sound).

Only transverse waves can be polarised because polarisation restricts the oscillation to a single plane; this is only meaningful when the oscillation is perpendicular to the travel direction, so there is a plane to choose. A longitudinal wave oscillates along the travel direction, so there is no perpendicular plane to restrict.

Markers reward the perpendicular versus parallel oscillation distinction, valid examples, and the polarisation reasoning.

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