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Wave-particle duality and de Broglie: WACE Year 12 Physics Unit 4

Syllabus dot point

“Explain wave-particle duality and apply the de Broglie wavelength to matter”

8 min read

Quick answer

Light behaves as a wave (interference, diffraction) and as particles (the photoelectric effect), depending on the experiment. De Broglie proposed that matter is the same, with any particle of momentum pp having a wavelength λ=hp=hmv\lambda=\dfrac{h}{p}=\dfrac{h}{mv}. Electron diffraction confirms this: electrons fired at a crystal form a diffraction pattern, a wave behaviour, proving matter has a wave nature.

What this dot point is asking

WACE wants you to explain that wave and particle models are complementary, apply the de Broglie relation, and cite electron diffraction as evidence. This dot point unifies the wave and photon strands of the unit.

Duality of light

The wave model explains interference, diffraction and polarisation, while the particle (photon) model explains the photoelectric effect and the line spectra of atoms. Neither model alone covers all observations, so light is described as having a dual nature: it shows wave properties in some experiments and particle properties in others, but never both in the same measurement.

De Broglie's matter waves

Louis de Broglie reasoned that if waves can act as particles, particles might act as waves. He assigned every moving particle a wavelength

λ=hp=hmv,\lambda=\frac{h}{p}=\frac{h}{mv},

where p=mvp=mv is the momentum and hh is Planck's constant. Because hh is tiny, the wavelength is utterly negligible for everyday objects, which is why a cricket ball shows no wave behaviour. For light, fast particles such as electrons it becomes comparable to atomic spacings and measurable.

Why everyday objects show no wave behaviour

A moving car has a de Broglie wavelength around 10−38 m10^{-38}\ \text{m}, far smaller than any aperture it could pass through, so it never diffracts. An electron accelerated through a modest voltage has a wavelength near 10−10 m10^{-10}\ \text{m}, similar to the spacing of atoms in a crystal, so a crystal acts as a diffraction grating for it.

Electron diffraction as evidence

When a beam of electrons is fired at a thin crystal or graphite film, it produces concentric diffraction rings on a screen, exactly the pattern expected when waves pass through a regular array of slits. Particles alone could not interfere to form rings, so this confirms that matter has a wave nature, validating de Broglie's idea.

De Broglie wavelength of an electron

Wavelength of an accelerated electron

An electron (m=9.11×10−31 kgm=9.11\times10^{-31}\ \text{kg}) moves at 3.0×106 m s−13.0\times10^6\ \text{m s}^{-1}. Find its de Broglie wavelength (h=6.63×10−34 J sh=6.63\times10^{-34}\ \text{J s}).

Momentum:

p=mv=(9.11×10−31)(3.0×106)=2.73×10−24 kg m s−1.p=mv=(9.11\times10^{-31})(3.0\times10^6)=2.73\times10^{-24}\ \text{kg m s}^{-1}.

Wavelength:

λ=hp=6.63×10−342.73×10−24=2.4×10−10 m.\lambda=\frac{h}{p}=\frac{6.63\times10^{-34}}{2.73\times10^{-24}}=2.4\times10^{-10}\ \text{m}.

This is about the spacing of atoms in a crystal, which is why such electrons diffract and slow everyday objects do not.

From accelerating voltage to wavelength

A very common multi-step question gives an accelerating voltage and asks for the de Broglie wavelength, chaining several relationships. The reliable route is: find the kinetic energy gained, Ek=qVE_k=qV; convert to speed using Ek=12mv2E_k=\tfrac{1}{2}mv^2, so v=2qV/mv=\sqrt{2qV/m}; find the momentum p=mvp=mv; then apply λ=h/p\lambda=h/p. A useful shortcut is to combine these into λ=h2mqV\lambda=\dfrac{h}{\sqrt{2mqV}}, which goes straight from voltage to wavelength in one substitution. This shows the wavelength falls as the accelerating voltage rises, which is exactly why electron microscopes use high voltages: a shorter de Broglie wavelength gives finer resolving power than visible light.

Complementarity: one model at a time

A subtle but examinable point is that wave and particle behaviours are complementary, never observed simultaneously. In a given experiment light (or matter) reveals either its wave nature or its particle nature, depending on what is being measured, but no single measurement shows both at once. The double-slit experiment shows interference (wave) when you do not detect which slit the light went through; the photoelectric effect shows discrete photons (particle) when light exchanges energy with electrons. The two pictures are not contradictory but together provide a complete description, with each appropriate to different situations. Stating that the models are complementary, and giving one wave experiment and one particle experiment as examples, is exactly the structure high-band duality answers use.

Using the relation correctly

Use λ=h/mv\lambda=h/mv with momentum in kg m s−1\text{kg m s}^{-1}, and remember that a larger momentum gives a shorter wavelength. If a voltage is given instead of a speed, first find the speed from qV=12mv2qV=\tfrac{1}{2}mv^2, then the momentum.

Applying photon energy E = hf to matter waves

The relation E=hfE=hf is for photons; for a matter wave you use λ=h/mv\lambda=h/mv to find its wavelength from momentum. Treating an electron as if it had a photon-style energy from its de Broglie frequency mixes the two pictures. For matter, start from momentum, not frequency.

Exam-style questions

Questions in the style of SCSA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

WACE 2023-style7 marks
An electron is accelerated from rest through a potential difference of 120 V120\ \text{V}. (a) Calculate the speed of the electron. (b) Calculate its de Broglie wavelength. (c) Explain why electrons of this wavelength can be diffracted by a crystal but a moving tennis ball cannot.
Show worked answer →

A 7 mark calculation rewards the speed from energy, the de Broglie wavelength and a comparison.

(a) Speed
qV=12mv2qV=\tfrac{1}{2}mv^2, so v=2qVm=2(1.6×10−19)(120)9.11×10−31=6.5×106 m s−1v=\sqrt{\dfrac{2qV}{m}}=\sqrt{\dfrac{2(1.6\times10^{-19})(120)}{9.11\times10^{-31}}}=6.5\times10^{6}\ \text{m s}^{-1}.
(b) Wavelength
p=mv=(9.11×10−31)(6.5×106)=5.9×10−24 kg m s−1p=mv=(9.11\times10^{-31})(6.5\times10^{6})=5.9\times10^{-24}\ \text{kg m s}^{-1}, so
λ=hp=6.63×10−345.9×10−24=1.1×10−10 m.\lambda=\frac{h}{p}=\frac{6.63\times10^{-34}}{5.9\times10^{-24}}=1.1\times10^{-10}\ \text{m}.
(c) Why the comparison
This wavelength is comparable to the atomic spacing in a crystal (∼10−10 m\sim10^{-10}\ \text{m}), so the crystal acts like a diffraction grating and the electrons diffract. A tennis ball has a huge momentum, so its de Broglie wavelength is around 10−34 m10^{-34}\ \text{m}, far smaller than any gap it could pass through, so no diffraction is observable.

Markers reward v=2qV/mv=\sqrt{2qV/m}, λ=h/(mv)\lambda=h/(mv) near 1.1×10−10 m1.1\times10^{-10}\ \text{m} and the wavelength-versus-aperture comparison for the two objects.

WACE 2021-style5 marks
Explain what is meant by wave-particle duality, and describe one piece of evidence for the wave nature of matter and one for the particle nature of light.
Show worked answer →

A 5 mark explanation needs the duality idea and one example each way.

Duality
Wave-particle duality is the idea that both light and matter can display wave-like behaviour in some experiments and particle-like behaviour in others. No single experiment shows both at once, but a complete description needs both models.
Wave nature of matter
Electron diffraction: a beam of electrons fired at a thin crystal produces concentric diffraction rings, a pattern only waves can produce by interference, showing matter has a wave nature with wavelength λ=h/mv\lambda=h/mv.
Particle nature of light
The photoelectric effect: light ejects electrons from a metal only above a threshold frequency, and the maximum electron energy depends on frequency not intensity, explained only if light arrives as discrete photons of energy E=hfE=hf.

Markers reward the complementary-models definition, electron diffraction for matter waves and the photoelectric effect for light as photons.

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