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Q.Complete the ray diagram for the incident rays OAOA, OA1OA_1, OA2OA_2, OA3OA_3.

Meghalaya MboseMBOSE Meghalaya Intermediate Board 2022Subjective· 2mImportance★★★★★
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Below the critical angle the rays simply refract into air, bending away from the normal; exactly at the critical angle the refracted ray grazes the surface; beyond the critical angle the ray cannot escape into air at all and undergoes total internal reflection back into the water.

Governing rule

For light going from a denser medium (water) to a rarer medium (air), Snell's law gives sin⁡r=μsin⁡i\sin r=\mu\sin i (with r>ir>i, μ=awn\mu={}^aw n). The critical angle CC is defined by sin⁡C=1/μ\sin C=1/\mu — the angle of incidence for which the refracted ray just grazes the surface (r=90∘r=90^\circ). The four rays sample every regime:

  • Ray OAOA (smallest ii, i<Ci<C): refracts into air, bending away from the normal, at a moderate refraction angle r>ir>i well short of 90∘90^\circ.
  • Ray OA1OA_1 (larger ii, still i<Ci<C): also refracts into air away from the normal, but at a larger refraction angle than OAOA's (closer to grazing, since ii is closer to CC).
  • Ray OA2OA_2 (i=Ci=C exactly): the refracted ray bends all the way to r=90∘r=90^\circ — it grazes along the water surface itself.
  • Ray OA3OA_3 (i>Ci>C): Snell's law would need sin⁡r=μsin⁡i>1\sin r=\mu\sin i>1, impossible — no refracted ray exists. Instead all the light undergoes total internal reflection: it reflects back down into the water, with angle of reflection == angle of incidence ii, on the other side of the normal at A3A_3. …

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