22.3 Wave–particle duality
- Syllabus
- 9702–2028–2029
- Topic
- 22.3
- Level
- A2
Wave-particle duality means electromagnetic radiation shows wave-like behavior in some observations and particle-like behavior in others; neither classical picture alone explains all evidence.
Photoelectric effect → particulate evidence: energy arrives in photons E=hf. A threshold frequency, immediate emission and Kmax depending on frequency rather than intensity follow from one-electron/one-photon transfer.
Interference and diffraction → wave evidence: overlapping alternatives produce stable maxima and minima through constructive and destructive superposition.
Dim radiation above threshold can eject electrons immediately, while bright sub-threshold radiation cannot; yet the same electromagnetic radiation can form interference fringes or diffract through an aperture.
Duality is not light physically switching between two substances. It is an evidence-based rule about which model predicts the measured outcome.
When electrons pass through a thin crystal or narrow spacing, they can form diffraction patterns rather than only particle-like spots.
The pattern is explained by a wavelength associated with the moving electrons; changing electron momentum changes the spacing of maxima and minima.
A ring pattern from a polycrystalline film is evidence of constructive interference from many crystal orientations.
Diffraction does not say an electron is a classical water wave; it reveals wave-like interference in the probability description.
A particle with momentum p has de Broglie wavelength λ=h/p, so greater momentum means a shorter wavelength.
For a non-relativistic electron p=mv; use the momentum actually delivered by the apparatus, not simply the particle’s rest mass.
Accelerating an electron through a larger potential difference increases its speed and reduces λ, changing the diffraction scale.
The wavelength is not a path the particle visibly traces; it predicts the scale of interference and diffraction effects.
Use λ=h/p with h=6.63×10⁻³⁴ J s and momentum p in kg m s⁻¹.
If speed is known and v is far below c, calculate p=mv first; keep units consistent before comparing λ with a slit or lattice spacing.
For a 9.11×10⁻³¹ kg electron moving at 2.0×10⁶ m s⁻¹, λ is about 0.36 nm, comparable with atomic spacings.
Do not substitute kinetic energy directly for p unless you first use the appropriate relation; rounding p too early can distort λ.