According to Snell’s law -
n₁ sin θ₁ = n₂ sin θ₂ given, θ₁ = 47.0°
For the refraction of violet light ( n = 1.66 ) from air to
glass
So, ( 1.00 ) sin 47.0° = ( 1.66 ) sin θ₂₁
=> sin θ₂₁ = ( 1.00 / 1.66 ) sin 47.0°
=> θ₂₁ = sin ⁻ ¹ [ ( 1.00 / 1.66 ) sin 47.0° ] = 26.1°
Now, for the refraction of violet light from glass to air
n₂ sin θ₂ = n₃ sin θ₃₁
heree, n₂ = 1.66, θ₂ = 60 - 26.1° =33.9o , n₃ =
1.00
=> sin θ₃₁ = ( n₂ / n₃ ) sin θ₂ = n₂ sin θ₂₂ = ( 1.66 ) sin
33.9°
… θ₃₁ = sin ⁻ ¹ [ ( 1.66 ) sin 33.9° ] = 67.8°
Again, for the refraction of red light ( n = 1.62 ) from air to glass -
=> ( 1.000 ) sin 47° = ( 1.62 ) sin θ₂
=> sin θ₂ = ( 1.000 / 1.62 ) sin 47°
=> θ₂ = sin ⁻ ¹ [ ( 1.000 / 1.62 ) sin 47° ] = 26.8°
For the refraction of red light from glass to air -
n₂ sin θ₂ = n₃ sin θ₃₂ given that, n₂ = 1.62, θ₂ = 26.8°, n₃ =
1.00
=> sin θ₃₂ = ( n₂ / n₃ ) sin θ₂ = n₂ sin θ₂ = ( 1.62 ) sin
26.8°
=> θ₃₂ = sin ⁻ ¹ [ ( 1.62 ) sin 26.8° ] = 47°
Therefore, γ = θ₃₁ - θ₃₂ = 67.8 - 47 = 20.8°
The index of refraction for violet light in silica flint glass is 1.66 and that for...
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