Images from Spherical Mirrors — Question 9

Section 34-4 · Physics pages 5628–5629

Question 9 Moving a curved mirror shifts its image by more than the mirror displacement Use the paraxial mirror relations 1/p + 1/q = 1/f and m = −q/p, with p positive for a real object, q positive for a real image, and f positive for a concave mirror. A fixed object is at laboratory coordinate x=0. A concave mirror at x=X faces the object, with constant focal length f and X greater than f. Its real image has laboratory coordinate xI = X −q, where p=X. F C V ˙X Schematic; labels, not drawing lengths, specify the data. (a) Derive the image velocity for a slowly translating mirror. (b) Evaluate the velocity ratio when X=3f, and compare with the plane-mirror limit at fixed X.
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Question 9 - Solution Moving a curved mirror shifts its image by more than the mirror displacement F C V ˙X (a) Method and calculation q = fX X −f , dq dX = − f2 (X −f)2 . vI = ˙X [ 1 + f2 (X −f)2 ] . (b) Interpretation and further calculation X = 3f ⇒vI/ ˙X = 5/4 . |f| →∞at fixed X : vI/ ˙X →2 . Physical check The plane limit continues the signed mirror formula to a virtual image; image coordinates must be converted back to the laboratory frame.

Question 9

Moving a curved mirror shifts its image by more than the mirror displacement

Use the paraxial mirror relations 1/p+1/q=1/f1/p+1/q=1/f and m=−q/pm=-q/p, with p positive for a real object, q positive for a real image, and f positive for a concave mirror. A fixed object is at laboratory coordinate x=0. A concave mirror at x=X faces the object, with constant focal length f and X greater than f. Its real image has laboratory coordinate xI=X−qx_I=X-q, where p=X.

Diagram shown in the original SVG worksheet.

  1. Derive the image velocity for a slowly translating mirror.

  2. Evaluate the velocity ratio when X=3f, and compare with the plane-mirror limit at fixed X.

Question 9 - Solution

Moving a curved mirror shifts its image by more than the mirror displacement

Diagram shown in the original SVG worksheet.

(a) Method and calculation

q=fXX−f,dqdX=−f2(X−f)2.q=\frac{fX}{X-f},\quad\frac{dq}{dX}=-\frac{f^2}{(X-f)^2}.vI=Ẋ[1+f2(X−f)2].\boxed{v_I=\dot X\left[1+\frac{f^2}{(X-f)^2}\right]}.

(b) Interpretation and further calculation

X=3f⇒vI/Ẋ=5/4.X=3f\Rightarrow\boxed{v_I/\dot X=5/4}.|f|→∞at fixed X:vI/Ẋ→2.|f|\to\infty\ \text{at fixed }X:\quad\boxed{v_I/\dot X\to2}.

Physical check

The plane limit continues the signed mirror formula to a virtual image; image coordinates must be converted back to the laboratory frame.