Spherical Mirrors — Question 1

Section 34-3 · Physics pages 5592–5593

Question 1 A source at the center of a sphere sends every reflected ray back along itself A concave spherical mirror is part of a sphere of radius R. A point source is exactly at the center of curvature C. The surrounding medium is homogeneous with light speed v. F C V Schematic; labels, not drawing lengths, specify the data. (a) Use the local surface normal to find the reflected direction for every ray reaching the mirror. (b) Find the round-trip optical travel time to C and its spread between rays striking different mirror heights.
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Question 1 - Solution A source at the center of a sphere sends every reflected ray back along itself F C V (a) Method and calculation ˆn = rhit −rC R , ˆki = ˆn. ˆkr = ˆki −2(ˆki · ˆn)ˆn = −ˆki . (b) Interpretation and further calculation ℓround = 2R, tround = 2R/v . ∆t = 0 for the ideal spherical surface and point source. Physical check This exact return property uses radial incidence and does not rely on the paraxial approximation.

Question 1

A source at the center of a sphere sends every reflected ray back along itself

A concave spherical mirror is part of a sphere of radius R. A point source is exactly at the center of curvature C. The surrounding medium is homogeneous with light speed v.

Diagram shown in the original SVG worksheet.

  1. Use the local surface normal to find the reflected direction for every ray reaching the mirror.

  2. Find the round-trip optical travel time to C and its spread between rays striking different mirror heights.

Question 1 - Solution

A source at the center of a sphere sends every reflected ray back along itself

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n̂=𝒓hit−𝒓CR,k̂i=n̂.\hat n=\frac{\mathbf r_{\mathrm{hit}}-\mathbf r_C}{R},\quad\hat k_i=\hat n.k̂r=k̂i−2(k̂i⋅n̂)n̂=−k̂i.\hat k_r=\hat k_i-2(\hat k_i\cdot\hat n)\hat n=\boxed{-\hat k_i}.

(b) Interpretation and further calculation

ℓround=2R,tround=2R/v.\boxed{\ell_{\mathrm{round}}=2R,\quad t_{\mathrm{round}}=2R/v}.Δt=0for the ideal spherical surface and point source.\boxed{\Delta t=0}\quad\text{for the ideal spherical surface and point source}.

Physical check

This exact return property uses radial incidence and does not rely on the paraxial approximation.