Diffraction
1. What Diffraction Is (vs Interference)
Diffraction = bending of light around edges/obstacles and spreading into geometrical shadow, due to interference of many coherent secondary wavelets from different parts of the same wavefront (Huygens–Fresnel principle).
- Interference: superposition of two separate beams (few sources) → equally spaced fringes with all maxima equal intensity.
- Diffraction: superposition of continuous secondary sources across one aperture → envelope with decreasing maxima, central brightest, with minima at different angles; fringe width not equal, intensities fall off.
Both are interference at heart, but diffraction is interference within one wavefront.
2. Huygens–Fresnel Principle
Every point on a wavefront acts as a secondary source; disturbance at is sum of secondary wavelets:
Phase depends on path length; amplitude ~ aperture function.
3. Two Types
- Fresnel diffraction: source and screen at finite distances, wavefronts spherical, no lenses; maths harder (Fresnel zones).
- Fraunhofer diffraction: source and screen at effective infinity (plane waves, lens focuses) → far-field, easier Fourier-type: pattern is Fourier transform of aperture.
Next topics focus on Fraunhofer.
4. Why Shadows Not Sharp
If wavelength aperture , diffraction spread tiny ⇒ shadow sharp (geometric optics limit). If , spread large ⇒ noticeable bending (this is why sound diffracts around doors but light not around buildings).
5. Worked Intuition
A 0.1 mm slit with λ=600 nm: first minima at θ≈ λ/a =6 mrad (≈0.34°) — measurable spread.
A hair vs radio wave: λ hair? Optical λ ~500 nm vs hair 50 µm: a≫λ ⇒ small diffraction; radio λ ~1 m vs building 10 m: a≈λ ⇒ strong diffraction around building.
6. Exam Points
- Define diffraction and distinguish from interference — 5 marks, very frequent (table comparison).
- State Huygens–Fresnel principle — 3-5 marks, frequent.
- Fresnel vs Fraunhofer with diagram (lenses vs not) — 5 marks, very frequent.
- Explain why geometrical shadow not perfectly sharp — 3 marks.