The Escape Angle

Critical angle — where refraction dies and reflection takes over

Setting up the lab…

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Selina ICSE: Refraction of Light at Plane Surfaces

What this lesson covers

Why it matters

Shine a torch UP from underwater. Tilt it slowly… and at one exact angle the light stops leaving the water at all. The surface becomes a perfect mirror.

The idea in plain words

The escape condition. Tap each term.

sin C = 1 ÷ μ

Find the critical angle for diamond (μ = 2.42).

C ≈ 24.4° — tiny! Light entering a cut diamond can barely escape, so it bounces and sparkles

  • degrees: C — critical angle — incidence (in the DENSER medium) for which r = 90°
  • no unit: μ — refractive index of the denser medium
  • the consequence: TIR — total internal reflection: beyond C, ALL light reflects — brighter than any mirror
  • sin C = 1 ÷ 2.42 = 0.413
  • C = sin⁻¹(0.413)

Predict first

Light inside glass (μ = 1.5) hits the surface at 50° from the normal. What happens?

For glass C = sin⁻¹(1/1.5) ≈ 41.8°. Beyond that, sin r would have to exceed 1 — impossible — so 100% of the light reflects: total internal reflection.

  • It is totally reflected back inside — 50° is beyond the critical angle — correct
  • It escapes, bending away from the normal
  • It escapes along the surface

What you do

Sweep the underwater torch. Find the exact angle where the escaping ray dies — then find it again for a second medium.

Check yourself

Total internal reflection needs…

Both conditions matter: dense → rare AND beyond the critical angle. No silver involved — the surface itself does it, losslessly.

Exactly AT the critical angle, the refracted ray…

C is defined by r = 90° — the escaping ray grazes the surface before TIR takes over.

A mirage on a hot road is caused by…

Hot air near the tar is optically rarer; sky-light curving through it TIRs upward — you see the sky and read it as water.

  • light going from denser to rarer, at i > C — correct
  • light going from rarer to denser at any angle
  • a silvered surface
  • skims along the surface (r = 90°) — correct
  • disappears
  • goes straight up the normal
  • gradual refraction + total internal reflection in layers of hot, rarer air — correct
  • water actually condensing on the road
  • sunlight reflecting off tar
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