Reflection and Refraction — Question 2

Section 33-7 · Physics pages 5494–5495

Question 2 Rotating a plane mirror doubles the reflected-ray rotation In a fixed two-dimensional laboratory plane, a ray arrives with propagation direction angle alpha. A plane mirror has tangent direction angle beta. Angles are signed counterclockwise from a fixed axis; the ray stays on the same reflecting face during a small mirror rotation. original and rotated mirror Schematic; labels, not drawing lengths, specify the data. (a) Derive the reflected propagation direction angle in terms of alpha and beta. (b) If the mirror rotates counterclockwise by 3 degrees while the incident direction is fixed, find the outgoing rotation. Find its sign if instead only the incident direction rotates by 3 degrees.
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Question 2 - Solution Rotating a plane mirror doubles the reflected-ray rotation original and rotated mirror (a) Method and calculation kr = ki −2(ki · ˆn)ˆn, αr = 2β −α (mod 2π) . dαr = 2 dβ −dα. (b) Interpretation and further calculation dα = 0, dβ = 3◦⇒dαr = 6◦. dβ = 0, dα = 3◦⇒dαr = −3◦. Physical check The factor of two refers to mirror rotation with the incoming ray fixed, not to a changing incident ray at a fixed mirror.

Question 2

Rotating a plane mirror doubles the reflected-ray rotation

In a fixed two-dimensional laboratory plane, a ray arrives with propagation direction angle alpha. A plane mirror has tangent direction angle beta. Angles are signed counterclockwise from a fixed axis; the ray stays on the same reflecting face during a small mirror rotation.

Diagram shown in the original SVG worksheet.

  1. Derive the reflected propagation direction angle in terms of alpha and beta.

  2. If the mirror rotates counterclockwise by 3 degrees while the incident direction is fixed, find the outgoing rotation. Find its sign if instead only the incident direction rotates by 3 degrees.

Question 2 - Solution

Rotating a plane mirror doubles the reflected-ray rotation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝒌r=𝒌i−2(𝒌i⋅n̂)n̂,αr=2β−α(mod⁡2π).\mathbf k_r=\mathbf k_i-2(\mathbf k_i\cdot\hat n)\hat n,\quad\boxed{\alpha_r=2\beta-\alpha\pmod{2\pi}}.dαr=2dβ−dα.d\alpha_r=2\,d\beta-d\alpha.

(b) Interpretation and further calculation

dα=0,dβ=3∘⇒dαr=6∘.d\alpha=0,\ d\beta=3^\circ\Rightarrow\boxed{d\alpha_r=6^\circ}.dβ=0,dα=3∘⇒dαr=−3∘.d\beta=0,\ d\alpha=3^\circ\Rightarrow\boxed{d\alpha_r=-3^\circ}.

Physical check

The factor of two refers to mirror rotation with the incoming ray fixed, not to a changing incident ray at a fixed mirror.