What is the relation between the refractive index of core n1 and cladding n2?
n2 is less than n1
Optical fibers are thin strands of glass or plastic used to transmit light signals over long distances. A typical optical fiber consists of two main parts: the core and the cladding.
Light travels through the optical fiber by a phenomenon called Total Internal Reflection (TIR). For TIR to occur at the boundary between the core and the cladding, the refractive index of the core must be greater than the refractive index of the cladding. The refractive index is a measure of how much light bends when it enters a medium. A higher refractive index means light bends more towards the normal when entering from a medium with a lower refractive index, or bends away from the normal when entering from a medium with a higher refractive index.
Let \(n_1\) be the refractive index of the core and \(n_2\) be the refractive index of the cladding.
For light rays propagating within the core to be reflected back into the core at the interface with the cladding, the condition for Total Internal Reflection must be met. This condition is that the refractive index of the first medium (where light is traveling) must be greater than the refractive index of the second medium (where reflection occurs). In the case of an optical fiber, light travels in the core and is reflected at the core-cladding interface. Therefore, the refractive index of the core (\(n_1\)) must be greater than the refractive index of the cladding (\(n_2\)).
Mathematically, the required relation for light guidance through TIR is:
\(n_1 > n_2\)
This inequality can also be stated as:
\(n_2 < n_1\)
This means that the cladding always has a lower refractive index than the core in a standard optical fiber designed for transmitting light signals via TIR.
| Part | Refractive Index | Function |
|---|---|---|
| Core (n1) | Higher refractive index | Carries the light signal |
| Cladding (n2) | Lower refractive index | Causes Total Internal Reflection, keeping light in the core |
Considering the options provided:
Option 1: n2 is less than n1 (\(n_2 < n_1\)) - This matches the condition \(n_1 > n_2\) required for TIR.
Option 2: n1 is equal to n2 (\(n_1 = n_2\)) - If refractive indices were equal, light would not reflect back into the core; it would likely pass into the cladding.
Option 3: n1 is less than n2 (\(n_1 < n_2\)) - If the core had a lower refractive index than the cladding, TIR could not occur at the core-cladding boundary for light traveling from core to cladding.
Option 4: No relation between n1 and n2 - There is a specific and essential relation for the optical fiber to function based on TIR.
Thus, for effective light transmission through an optical fiber via Total Internal Reflection, the refractive index of the cladding (\(n_2\)) must be less than the refractive index of the core (\(n_1\)).
| Property | Core | Cladding |
|---|---|---|
| Refractive Index | \(n_1\) (Higher) | \(n_2\) (Lower) |
| Role in Light Propagation | Guides light | Confines light via TIR |
Total Internal Reflection occurs when light travels from a medium with a higher refractive index to a medium with a lower refractive index, and the angle of incidence exceeds a critical angle. The critical angle (\(\theta_c\)) is given by Snell's Law:
\(\sin(\theta_c) = \frac{n_2}{n_1}\)
where \(n_1\) is the refractive index of the denser medium (core) and \(n_2\) is the refractive index of the rarer medium (cladding). For TIR to happen, \(n_1 > n_2\) is a necessary condition.
In an optical fiber, light enters the core and strikes the core-cladding boundary at angles greater than the critical angle, ensuring it reflects back into the core and continues to travel along the fiber.
Fibre optic power meters have input for attaching fiber optic connector and detector:
Graded index fiber is used to
A graded indexed optical fiber has a parabolic refractive index profile (α = 2). If the fiber has a numerical aperture = 0.22 the total number of guided modes at a wavelength of 1310 nm is given by:
In optical fibers, following statements are given:
(A) \(\rm\frac{1}{v_s} = −\frac{λ^2}{2 \pi c} \frac{d b}{d λ}\)
(B) v g= \(\rm −\frac{λ^2}{2 \pi c}\) dβ/dλ
(C) D = \(\rm −\frac{2 \pi c}{\pi^2}\) β 2
(D) β 2= \(\rm −\frac{2 \pi c}{\pi^2}\) . D
(E) Material dispersion is a function of (λ) wavelength
Choose the correct answer from the options given below:
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