Physics · Ch 9 — Ray Optics and Optical Instruments
Total Internal Reflection
Total Internal Reflection
When light travels from an optically denser medium towards a rarer medium (for example, from glass or water towards air), Snell's law shows the refracted ray bends away from the normal, so the angle of refraction is always larger than the angle of incidence . As is increased, increases faster, and at one particular angle of incidence -- the critical angle -- the refracted ray grazes along the boundary itself, emerging at . For any angle of incidence greater than this critical angle, no refracted ray can exist at all (Snell's law would require , which is impossible), and the entire incident ray is reflected back into the denser medium, obeying the ordinary laws of reflection exactly. This phenomenon is called total internal reflection (TIR), and unlike reflection from a silvered mirror, it reflects essentially 100% of the incident light, with no absorption loss at all. Two conditions must both hold for TIR to occur: light must be travelling from a denser medium towards a rarer medium (never the other way round), and the angle of incidence inside the denser medium must exceed the critical angle for that pair of media. The critical angle itself follows directly from Snell's law by setting : for a ray going from a medium of refractive index towards air (), A denser medium (larger ) therefore has a smaller critical angle, i.e. TIR happens more readily. Familiar demonstrations and applications of TIR include the brilliant sparkle of a cut diamond (diamond's very high refractive index, about , gives it an unusually small critical angle of about , so light entering the stone undergoes TIR repeatedly at its many facets before emerging), the mirage seen over a hot road or desert surface (light from the sky bends progressively in layers of air that grow hotter and less dense near the ground, undergoing something close to TIR and rea …
What this figure shows. One combined diagram, drawn as three separate rays all originating from the same point O just below a horizontal boundary line separating a denser medium below (shaded, labelled 'denser medium, e.g. glass, refractive index n') from a rarer medium above (unshaded, labelled 'rarer medium, e.g. air'), with a short vertical dashed normal line drawn through O perpendicular to the boundary. Ray 1, drawn at a small angle from the normal, crosses the boundary and bends away from the normal into the upper medium, showing ordinary refraction with the angle of refraction r1 marked larger than the angle of incidence i1. Ray 2, drawn at a larger angle of incidence C from the normal (labelled 'critical angle C'), crosses the boundary and travels exactly ALONG the boundary line itself, at a marked angle of exactly 90 degrees from the normal, illustrating the critical-angle case. Ray 3, drawn at an angle of incidence greater than C, does NOT cross the boundary at all -- instead it reflects back down into the lower medium at an angle equal to its angle of incidence, drawn with an arrowhead pointing back down into the denser medium and …