Propagation mechanism of light in fibre
1. Two Views — Ray vs Wave
- Ray (geometric) model: Light rays zig-zag via TIR (step-index) or bend sinusoidally (graded) — intuitive for large .
- Wave (mode) model: Fibre is cylindrical waveguide; Maxwell's equations with boundary at give discrete modes LP (like waveguide) with propagation constant (). Both views agree when many modes.
2. Ray Propagation (what exam expects)
- Step-index MMF: ray angle to axis, TIR at core-cladding requires ? Actually complementary. Axial ray shortest, extreme () longest path:
⇒ delay difference
per km (modal dispersion). This is why step MMF pulses spread.
- Graded-index: parabolic ⇒ ray equation gives sinusoidal trajectory with period
focusing, so all modes have nearly equal group velocity ⇒ low dispersion.
- Single-mode: only one ray (fundamental mode) ⇒ no modal dispersion.
3. Wave Modes
For step fibre, solving Helmholtz in cylindrical coordinates with Bessel in core, in cladding, continuity gives eigenvalue equation whose solutions are modes. Count ≈ for large ; cutoff for LP11.
- Mode field diameter slightly larger than core for SMF.
- Effective index .
4. Polarization and Evanescent Field
Total internal reflection leaves evanescent field in cladding decaying as over ~; cladding must be thick enough (≥ few µm) to prevent loss to coating.
5. Worked Intuition
Step-index fibre length 1 km, n1=1.48, Δ=0.01: Δτ≈ n1 L Δ /c ≈1.48·1000·0.01/3e8≈49 ns (step) vs GRIN Δτ≈ n1 L Δ²/8c≈0.06 ns (real).
6. Exam Points
- Describe ray propagation via TIR (step) vs sinusoidal (graded) — 5 marks, very frequent.
- Mention mode view and estimate — 3-5 marks, frequent.
- Explain modal dispersion due to path length difference — 5 marks, very frequent.
- Evanescent field in cladding — 3 marks.