Reflection of a plane wave: proving the law of reflection
Using Huygens' wavelets on a mirror, the two triangles formed are congruent, so the angle of incidence equals the angle of reflection.
Proof of the law of reflection
A plane wavefront AB falls on a plane reflecting surface MN at an angle i. Light travels at speed v in the medium.
- 1End A of the wavefront touches the surface first. End B still has to travel a distance BC to reach the surface at C.
- 2Let this take a time τ. Then BC = vτ.
- 3In the same time τ, a secondary wavelet from A spreads back into the same medium. Its radius is AE = vτ.
- 4From C, draw a tangent CE to this wavelet, touching it at E. CE is the reflected wavefront.
- 5In triangles ABC and AEC: AC is common, BC = AE = vτ, and ∠ABC = ∠AEC = 90°.
- 6So the two triangles are congruent (RHS rule). Hence ∠BAC = ∠ECA.
- 7∠BAC is the angle of incidence i, and ∠ECA is the angle of reflection r.The angle between a wavefront and the surface equals the angle between the ray and the normal, because both pairs are at 90°.
- 8★So, i = r: the angle of incidence equals the angle of reflection.
★ key step
How to draw the diagram for reflection
- Draw a horizontal line MN; label it reflecting surface.
- Draw the incident wavefront AB slanting down so that A touches MN. Mark the angle i between AB and MN.
- Draw two incident rays at right angles to AB: one reaching A, and one passing through B to meet MN at C. Write BC = vτ.
- With A as centre, draw an arc of radius vτ above MN.
- From C, draw a tangent CE to the arc; label it reflected wavefront. Mark the angle r between CE and MN.
- Draw reflected rays at right angles to CE, and dashed normals at A and C.
What happens to a plane wavefront in a prism, a lens and a mirror
| Device | Emerging wavefront | Why |
|---|---|---|
| Thin prism | Plane, but tilted towards the base | Light near the thick base spends longer in glass, where it is slower, so that part lags behind |
| Convex lens | Converging spherical, meeting at the focus | The middle part passes through the thickest glass and is delayed the most |
| Concave mirror | Converging spherical, meeting at the focus | The edges of the wavefront reach the curved mirror first and turn back earlier |
A DTH dish antenna on Indian rooftops is a curved reflector. It turns the plane wavefronts from a far-off satellite into converging wavefronts that meet at the receiver placed at its focus.
3 marks: “Use Huygens' principle to verify the law of reflection at a plane surface. Draw a labelled diagram.” Wavefront AB at angle i; BC = vτ; wavelet from A of radius AE = vτ; tangent CE is the reflected wavefront; triangles ABC and AEC congruent (RHS), so i = r; diagram with normals, i and r marked.
2 marks: “Draw the reflected wavefront when a plane wavefront falls on a concave mirror. Where does it go?” A converging spherical wavefront that shrinks to the focus F of the mirror. Diagram: parallel straight lines coming in, arcs centred on F going out.
1 marks: “A plane wavefront passes through a thin prism. What is the shape of the emerging wavefront?” Still plane, but tilted towards the base of the prism.
Same medium, same speed, same radius: BC = AE = vτ, so the triangles match and i = r.