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Light guidance in an optical fiber can b...

Light guidance in an optical fiber can be understood by considering a sturcture comprising of thin solid glass cylinderof refractive index `n_(1)` surrounded by a medium of lower refractive index `n_(2)`. The light guidance in the structure takes place due to successive total internal reflection at the interface of the media `n_(1)` and `n_(2)` as shown in the figure. All reys with the angle of incedence `i` less than a particular value `i_(m)` are confined in the medium of refractive index `n_(1)`. The numerical aperture `(NA)` of the structure is defined as `sin i_(m)`

If two structures of same cross-sectional area, but different numerical apertures `NA_(1)` and `NA_(2)` `(NA_(2)ltNA_(1))` are joined longitudinally, the numerical aperture of the combined structure is

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The correct Answer is:
D

It is given that
`implies i_(m2) lt i_(m1)`
Hence if the combination can be placed both ways i.e., `1^(st)` structure & then `2^(nd)` structure and then reversed also , then the condition of TIR is satisfied for lower `i_(m)` then it can satisfied for all other less angler as well.
Hence `NA_(2)` will be the numerical aperture of the combined structure .
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Light guidance in an optical fibre can be understood by considering a structure comprising of thin solid glass cylinder of refractive index n_1 surrounded by a medium of lower refractive index n_2 . The light guidance in the structure takes place due to successive total internal reflectrions at the interface of the media n_1 and n_2 as shown in the fugure. All rays with the angle of incidence i less than a particular value i_m are confined in the medium of refractive index n_1 . The numerical aprture (NA) of the structure is defined as sini_m If two structure of same cross-sectional area, but different numerical apertures NA_1 and NA_2(NA_2ltNA_1) are joined longitudinally, the numerical aperture of the combined structure is

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