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NotesPhysics HLTopic 5.2De Broglie wavelength and diffraction
Back to Physics HL Topics
5.2.22 min read

De Broglie wavelength and diffraction

IB Physics • Unit 5

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Contents

  • Particles are waves too
  • Electron diffraction — the evidence
  • Why don't everyday objects show it?
  • The uncertainty principle
  • In the exam
The big idea: If light (a wave) can act like a particle, then matter (particles) can act like a wave. De Broglie said every moving particle has a wavelength set by its momentum p — the bigger the momentum, the shorter the wavelength.
Given in the data booklet — the de Broglie wavelength (p = mv for a slow particle).
de Broglie wavelength (m)
Planck constant, 6.63×10⁻³⁴ J s
momentum of the particle (kg m s⁻¹)

Worked example — wavelength of an electron

An electron (mass 9.11 × 10⁻³¹ kg) moves at 2.0 × 10⁶ m s⁻¹. Find its de Broglie wavelength.

Solution

  1. First the momentum, then the given formula:
  2. Substitute into λ = h/p:
  3. Work it out — keep the unit:

Final answer

λ = 3.6 × 10⁻¹⁰ m — about the size of an atom, so it can diffract off crystals.

Electrons make diffraction patterns: Fire a beam of electrons at a thin crystal and you get a diffraction pattern of rings — exactly what waves do when they pass through gaps about the size of their wavelength.

The atomic spacing in the crystal (~10⁻¹⁰ m) matches an electron's de Broglie wavelength, so the effect shows up. This is direct proof that particles have a wave nature.

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Big, everyday objects have huge momentum, so their de Broglie wavelength is far too small to ever notice. Wave behaviour only shows up for tiny particles like electrons.

Worked example — a cricket ball

A 0.16 kg cricket ball is bowled at 40 m s⁻¹. Find its de Broglie wavelength, and comment.

Solution

  1. Momentum, then λ = h/p:
  2. Substitute:
  3. Compare: this is far smaller than any gap or atom, so no diffraction is ever observed.

Final answer

λ ≈ 1 × 10⁻³⁴ m — unimaginably small, so a cricket ball never behaves like a wave.

You can't have it both ways: Because particles behave as waves, you cannot know both a particle's position and its momentum exactly at the same time. The more precisely you pin down one, the less precisely you can know the other.
Given in the data booklet — Heisenberg's uncertainty principle (position–momentum).
uncertainty in position (m)
uncertainty in momentum (kg m s⁻¹)
Planck constant, 6.63×10⁻³⁴ J s

Worked example — minimum uncertainty

An electron's position is known to within Δx = 1.0 × 10⁻¹⁰ m. Find the minimum uncertainty in its momentum.

Solution

  1. At the minimum, the ≥ becomes =. Rearrange the given relation for Δp:
  2. Substitute:
  3. Work it out:

Final answer

Δp ≥ 5.3 × 10⁻²⁵ kg m s⁻¹.

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Where it shows up: Matter waves are HL only (E.2):

- Paper 1A — a quick λ = h/p, or 'why do electrons diffract but cricket balls don't?'. - Paper 2 — find a de Broglie wavelength (often after finding the momentum first), or a minimum uncertainty from Δx·Δp ≥ h/4π.
Three easy marks: (1) Find the momentum p = mv first, then λ = h/p. (2) A bigger momentum → a shorter wavelength. (3) Diffraction needs a gap about the size of the wavelength.

IB-style question — wavelength of a proton

A proton has a momentum of 3.0 × 10⁻²¹ kg m s⁻¹. Determine its de Broglie wavelength.

Solution

  1. Write the given formula first:
  2. Substitute:
  3. Work it out:

Final answer

λ = 2.2 × 10⁻¹³ m.

IB Exam Questions on De Broglie wavelength and diffraction

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How De Broglie wavelength and diffraction Appears in IB Exams

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Define

Give the precise meaning of key terms related to De Broglie wavelength and diffraction.

AO1
Describe

Give a detailed account of processes or features in De Broglie wavelength and diffraction.

AO2
Explain

Give reasons WHY — cause and effect within De Broglie wavelength and diffraction.

AO3
Evaluate

Weigh strengths AND limitations of approaches in De Broglie wavelength and diffraction.

AO3
Discuss

Present arguments FOR and AGAINST with a balanced conclusion.

AO3

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