According to de Broglie, every particle with momentum p behaves like a wave with wavelength
\$\lambda = \frac{h}{p}\$
Here h is Planck’s constant. For an electron moving at 1 × 10⁶ m s⁻¹, λ is about 0.001 nm – tiny, but still real!
⚛️ Setup: A beam of high‑energy electrons is fired at a thin metal foil (e.g., aluminium). The foil is so thin that electrons can pass through but still interact with the crystal lattice.
📐 Observation: On a screen behind the foil, a series of bright and dark rings (a diffraction pattern) appears, just like the pattern from light passing through a slit.
Imagine throwing a stone into a pond. The ripples spread out in concentric circles. If you place a grid of pegs in the water, the ripples will bend around them and create a pattern of bright and dark spots when viewed from above. Electrons behave in a similar way when they “ripples” through the crystal lattice.
Key Points to Remember:
💡 Tip: In exam questions, look for phrases like “diffraction pattern” or “interference” – they signal you should invoke wave behaviour.
| Feature | Wave Signature | Particle Signature |
|---|---|---|
| Diffraction Pattern | ✔️ Bright & dark rings | ✖️ No interference |
| Dependence on Energy | ✔️ Pattern shifts with voltage | ✖️ No energy‑dependent pattern |
| Relation to De Broglie Wavelength | ✔️ Consistent with λ = h/p | ✖️ Not applicable |