written 7.7 years ago by | • modified 7.7 years ago |
Mumbai University > Electronics and telecommunication > Sem 7 > optical communication and networks
Marks: 10
Years: MAY 2012
written 7.7 years ago by | • modified 7.7 years ago |
Mumbai University > Electronics and telecommunication > Sem 7 > optical communication and networks
Marks: 10
Years: MAY 2012
written 7.7 years ago by |
Determining Numerical Aperture for graded index fibers is more complex than for step index fibers, since it is a function of position across the core end face.
$\Rightarrow$ Graded Index Fiber does not have a constant refractive index in the core. Due to this property they are also called inhomogeneous core fibers.
$\Rightarrow$ It has a decreasing core index n(r) with radial distance from a maximum value of $n_1$ at the axis to a constant value $n_2$ beyond the core radius a in the cladding.
The index variation is given by
Where, r = radial distance from the fiber axis
a = core radius
$n_1 =$ refractive index at the core axis
$ Δ =$ relative refractive index difference
$Δ =\dfrac {n_1^2 - n_2 ^2}{2n_1^2} ≈ \dfrac {n_1- n_2}{n_1} $
$\alpha$ = profile parameter which gives the characteristics
Refractive index profile of the fiber core.
$\Rightarrow$ Light incident on the fiber core at position r propagates as guided mode if it is within local NA. The local NA is defined as:
Where the axial NA is defined as:
$NA(0)= n_1 \sqrt{2∆}$
Figure 1.6
$\Rightarrow $Thus, the NA of GIF decreases from NA (0) to 0 as r moves from fiber axis to core-cladding boundary.