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A light beam is travelling from Region I to Region IV as shown in the figure below: The refractive indices of Regions I, II, III and IV are ЁЭСЫ0,ЁЭСЫ02,ЁЭСЫ06 and ЁЭСЫ08 respectively.

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A light beam is travelling from Region I to Region IV as shown in the figure below: The refractive indices of Regions I, II, III and IV are `n_0, n_0/2,n_0/6` and `n_0/8` respectively. The angle of incidence θ for which the beam just misses entering Region IV is:

рд╡рд┐рдХрд▓реНрдк

  • `sin^-1 (3/4)`

  • `sin^-1 (1/8)`

  • `sin^-1 (1/4)`

  • `sin^-1 (1/3)`

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`bb(sin^-1 (1/8))`

Explanation:

Refractive indices:

Region I: n0

Region II: `n_0/2`

Region III: `n_0/6`

Region IV: `n_0/8`

sin θc = `(n_0/8)/(n_0/6) = 3/4`

Step 1: Critical angle at the region III–IV interface:

For the light ray to just enter region IV, it must strike the region III–IV boundary at the critical angle θcтАЛ:

`sin θ_c = n_4/n_3`

= `(n_0/8)/(n_0/6)`

= `6/8`

= `3/4`

Step 2: Apply Snell’s law from region I to III directly:

From region I to III (combining both interfaces), Snell’s law:

`n_0 sin θ = n_0/6 sin θ_c`

`sin θ = 1/6 xx sin θ_c`

= `1/6 xx 3/4`

= `1/8`

θ = `sin^-1 (1/8)`

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