Thin Lenses — Question 8

Section 34-6 · Physics pages 5666–5667

Question 8 A second lens collimates a real intermediate image Use the thin-lens relations 1/p + 1/q = 1/f and m = −q/p in one surrounding medium. Distances p and q are positive for real objects and real images; f is positive for a converging lens. Lens 1 has f1=10 cm and views an object at p1=15 cm. Lens 2, with f2=20 cm, is 50 cm to the right of lens 1. The original object height is 2 mm. d first second I1 Schematic; labels, not drawing lengths, specify the data. (a) Find the intermediate image and show that the final beam is collimated. (b) Find the intermediate signed image height and outgoing beam angle, using αout = −h1/f2.
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Question 8 - Solution A second lens collimates a real intermediate image d first second I1 (a) Method and calculation q1 = 10(15)/(15 −10) = 30 cm , p2 = 50 −30 = 20 cm = f2. 1/q2 = 1/f2 −1/p2 = 0 ⇒q2 →∞. (b) Interpretation and further calculation m1 = −30/15 = −2 ⇒h1 = −4 mm . αout = −(−4)/(200) = +0.020 rad . Physical check An image at infinity is described by outgoing direction rather than a finite final image height.

Question 8

A second lens collimates a real intermediate image

Use the thin-lens relations 1/p+1/q=1/f1/p+1/q=1/f and m=−q/pm=-q/p in one surrounding medium. Distances p and q are positive for real objects and real images; f is positive for a converging lens. Lens 1 has f1=10 cm and views an object at p1=15 cm. Lens 2, with f2=20 cm, is 50 cm to the right of lens 1. The original object height is 2 mm.

Diagram shown in the original SVG worksheet.

  1. Find the intermediate image and show that the final beam is collimated.

  2. Find the intermediate signed image height and outgoing beam angle, using αout=−h1/f2\alpha_{\mathrm{out}}=-h_1/f_2.

Question 8 - Solution

A second lens collimates a real intermediate image

Diagram shown in the original SVG worksheet.

(a) Method and calculation

q1=10(15)/(15−10)=30cm,p2=50−30=20cm=f2.q_1=10(15)/(15-10)=\boxed{30\,\mathrm{cm}},\quad p_2=50-30=20\,\mathrm{cm}=f_2.1/q2=1/f2−1/p2=0⇒q2→∞.1/q_2=1/f_2-1/p_2=0\Rightarrow\boxed{q_2\to\infty}.

(b) Interpretation and further calculation

m1=−30/15=−2⇒h1=−4mm.m_1=-30/15=-2\Rightarrow\boxed{h_1=-4\,\mathrm{mm}}.αout=−(−4)/(200)=+0.020rad.\boxed{\alpha_{\mathrm{out}}=-(-4)/(200)=+0.020\,\mathrm{rad}}.

Physical check

An image at infinity is described by outgoing direction rather than a finite final image height.