Spherical Refracting Surfaces — Question 1

Section 34-5 · Physics pages 5632–5633

Question 1 A single curved interface can form an enlarged real image Use n1/p + n2/q = (n2 −n1)/R and m = −n1q/(n2p) for paraxial refraction. Here p is positive on the incident side, q on the outgoing side, and R when the center lies on the outgoing side. Light passes from air n1=1.00 into glass n2=1.50 across a surface with R=+10 cm. The real object is at p=30 cm and has height 3 mm. C n1 n2 V Schematic; labels, not drawing lengths, specify the data. (a) Find the image distance and classify the image. (b) Find magnification and signed image height, retaining the index ratio.
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Question 1 - Solution A single curved interface can form an enlarged real image C n1 n2 V (a) Method and calculation 1.50 q = 0.50 10 −1 30 = 1 60 ⇒q = 90 cm . q > 0 ⇒real image in glass . (b) Interpretation and further calculation m = −1(90) 1.50(30) = −2 . hI = −2(3) = −6 mm . Physical check The transverse magnification for one refracting surface is not simply minus q/p when the two media differ.

Question 1

A single curved interface can form an enlarged real image

Use n1/p+n2/q=(n2−n1)/Rn_1/p+n_2/q=(n_2-n_1)/R and m=−n1q/(n2p)m=-n_1q/(n_2p) for paraxial refraction. Here p is positive on the incident side, q on the outgoing side, and R when the center lies on the outgoing side. Light passes from air n1=1.00 into glass n2=1.50 across a surface with R=+10 cm. The real object is at p=30 cm and has height 3 mm.

Diagram shown in the original SVG worksheet.

  1. Find the image distance and classify the image.

  2. Find magnification and signed image height, retaining the index ratio.

Question 1 - Solution

A single curved interface can form an enlarged real image

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1.50q=0.5010−130=160⇒q=90cm.\frac{1.50}{q}=\frac{0.50}{10}-\frac1{30}=\frac1{60}\Rightarrow\boxed{q=90\,\mathrm{cm}}.q>0⇒real image in glass.q>0\Rightarrow\boxed{\text{real image in glass}}.

(b) Interpretation and further calculation

m=−1(90)1.50(30)=−2.\boxed{m=-\frac{1(90)}{1.50(30)}=-2}.hI=−2(3)=−6mm.\boxed{h_I=-2(3)=-6\,\mathrm{mm}}.

Physical check

The transverse magnification for one refracting surface is not simply minus q/p when the two media differ.