Fibre Optics
Optical Fibre #
Has 3 coaxial regions
- Innermost region: light guiding region: core
- Middle region: cladding
- Surrounds the core
- Its refractive index is lower than the core
- Reduces scattering losses.
- Outermost region: Sheath/protective buffer/outer jacket
- Adds mechanical strength
They are constructed as either as a single fibre or a bundled up cable.
Snell’s Law #
$$ n_1 \sin i = n_2 \sin r $$
Total Internal Reflection #
The angle of incidence is such that the refracted angle goes to 90° and then turns into total internal reflection if it’s greater than the ‘critical angle’
$$ \sin i_c = \frac{n_2}{n_1}<1 $$
Light in a fibre optic travels by utilizing this property of reflection/refraction
Types of Optical Fibres #
There are 2 types:
- Single Mode Fibre (SMF): Has a smaller core diameter and can support only one mode of propagation.
- Multimode Fibre (MMF): Has a larger core diameter and supports a number of modes. Further distinguished based on index-profile
- Step index type
- Graded index (GRIN) type
Single Mode Step Index Fibre #
- Refractive index changes abruptly at the core-cladding boundary: “step index”
- Core diameter: 4 μm
- Path: Single and almost straight
- NA: 0.05-0.4
Multimode Step Index Fibre #
- Referactive index changes abruptly at the core-cladding boundary: “step index”
- Core diameter: 100 μm
- Path: Many zigzag paths
- NA: order of 3
Multimode Graded Index Fibre #
- Refractive index of the core varies with distance from the fibre axis. Has high value at the center and falls off with increasing radial distance from the axis.
- Acceptance angle and Numerical aperture decreases with radial distance from axis.
Parameters of Fibres #
Numerical Aperature #
There are three rays that are involved
- Incident ray going into the tube →
- Refracted ray bouncing the wall of the core →
- Totally internally reflected ray
i: Angle of the initial incident ray with respect to the axis of the tube
i_max: acceptance angle of incidence for which the total internal refraction can occur.
$$\sin i_{max}=\sqrt{n_1^2-n_2^2}=NA\approx n_1\sqrt{2\Delta}$$
$\Delta=\frac{n_1-n_2}{n_1}$
i_max: acceptance angle of incidence for which the total internal refraction can occur.
V-Number #
Called normalized frequency of the fibre.
a: radius of the core $$ V=\frac{2\pi a}{\lambda}NA $$
Maximum possible modes #
N_m: maximum number of modes supported
- by a Step Index fibre: $\frac{V^2}{2}$ (if V<2.405: N_m=1, else N_m>1)
- by a GRIN fibre: $\frac{V^2}{4}$
Losses in optical fibre #
For a fibre of length L and Power input P_i and output P_o,
loss = $\frac{10}{L} \log \frac{P_i}{P_o}$
Advantages (over coaxial cables) #
- No loss
- Speed/Bandwidth
- Cost effective
- Light weight
- Strong and flexible
- Non Hazardous
- Low Interference. No cross talk.
- Low/no electromagnetic and radio frequency interference
Applications #
- Medical applications
- A bundle of fibres (MMF) is used to illuminate areas of body
- A 2nd bundle is used to collect the reflected light
- A laser beam is also used as a guide in many cases.
- Military applications
- Maintains true communication silence to the enemy.
- Use of Fibre-guided missiles that send video and receive commands for operations
- Entertainment Applications
- For optical projection systems
- Optical Fibre Sensors: To measure
- Temperature changes
- Smoke/pollution detector
- Level of liquid in a container.
- Communications Applications