Thin Lenses — Question 3

Section 34-6 · Physics pages 5656–5657

Question 3 Unequal lens curvatures combine through their signed reciprocal radii A thin glass lens in air has index n=1.60. For left-to-right propagation, its radii are R1=+24 cm and R2=-40 cm, positive when a surface center lies to the right. Use 1/f = (n −1)(1/R1 −1/R2). F F ′ Schematic; labels, not drawing lengths, specify the data. (a) Find focal length and optical power in inverse meters. (b) Flip the lens end for end and show whether its thin-lens focal length changes.
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Question 3 - Solution Unequal lens curvatures combine through their signed reciprocal radii F F ′ (a) Method and calculation 1/f = 0.60(1/24 + 1/40) = 0.0400 cm−1. f = 25.0 cm = 0.250 m, P = 4.00 m−1 . (b) Interpretation and further calculation R′ 1 = +40 cm, R′ 2 = −24 cm. 1/f′ = 0.60(1/40 + 1/24) = 1/f ⇒f′ = f . Physical check Reversing a thin lens in the same medium leaves its paraxial power unchanged, though aberrations can depend on orientation.

Question 3

Unequal lens curvatures combine through their signed reciprocal radii

A thin glass lens in air has index n=1.60. For left-to-right propagation, its radii are R1=+24 cm and R2=-40 cm, positive when a surface center lies to the right. Use 1/f=(n−1)(1/R1−1/R2)1/f=(n-1)(1/R_1-1/R_2).

Diagram shown in the original SVG worksheet.

  1. Find focal length and optical power in inverse meters.

  2. Flip the lens end for end and show whether its thin-lens focal length changes.

Question 3 - Solution

Unequal lens curvatures combine through their signed reciprocal radii

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1/f=0.60(1/24+1/40)=0.0400cm−1.1/f=0.60(1/24+1/40)=0.0400\,\mathrm{cm^{-1}}.f=25.0cm=0.250m,𝒫=4.00m−1.\boxed{f=25.0\,\mathrm{cm}=0.250\,\mathrm m,\quad\mathcal P=4.00\,\mathrm{m^{-1}}}.

(b) Interpretation and further calculation

R1′=+40cm,R2′=−24cm.R_1^\prime=+40\,\mathrm{cm},\quad R_2^\prime=-24\,\mathrm{cm}.1/f′=0.60(1/40+1/24)=1/f⇒f′=f.1/f^\prime=0.60(1/40+1/24)=1/f\Rightarrow\boxed{f^\prime=f}.

Physical check

Reversing a thin lens in the same medium leaves its paraxial power unchanged, though aberrations can depend on orientation.