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Solutions to various problems related to image formation using mirrors and lenses. The problems cover topics such as plane and curved mirrors, concave and convex lenses, and magnification. Students can use these solutions to understand the concepts of image formation, mirror and lens equations, and magnification.
Typology: Lecture notes
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Mirrors Problem
Solution A small mirror (M) on the floor intercepts rays
traveling nearly parallel to the floor. The angle to the customer's eye (E) from the mirror is twice the angle of reflection, so tan 2a = h/d, or a = tan-' x (140150) = 35.2", for the given distances. Therefore, the plane of the mirror should be tilted by 35.2" from the vertical to provide the customer with a floor-level view of her shoes.
Problem 1 Solution.
Problem
Find the locations of all images of an object a t z = 2 m , y = l m.
FIGURE 36-44 Problem 2 Solution.
Solution In addition ,to the two direct images in each mirror (one reflection) at I, = (-2 m, 1 m) and I, = (2 m, -1 m), a multiple image (two reflections) also appears a t I,, = (-2 m, -1 m). (The latter is the image in one mirror of the direct image in the other.) Ray tracing confirms this, as shown on Fig. 36-44. No more than two reflections are possible for perpendicular mirror planes, so these are all the images.
Problem
Solution (a) The mirror equation relates the given distances (both positive for a real object and image) to the focal length: f-' = (50 cm)-I + (75 cm)-l, or f = 30 cm. (See Equation 36-2.) (b) A second application of the
virtual, erect image located behind the mirror. (Fig. 3 6 8 c and Table 36-1 confirm these results.)
Problem
Solution (a) The mirror equation (Equation 36-2) gives e = fr/(P1 - f ) = (18 cm)(-40 cm)/(-58 cm) = 12.4 cm (positive distances are in front of the mirror, negative distances behind). (b) Equation 36- 1 gives M = -el/t? = +40 cm112.4 cm = 3.22.
Problem.
Solution An upright image in a concave mirror must be virtual, so M = +3 = -el/!. The mirror equation gives ( i / e ) + ( i / r ) = ( l i e ) - (ij3e) = llf,or e = (g)f = ($)(27 cm) = 18 cm (positive in front of the mirror).
Problem
Solution The sphere reflects like a convex mirror of focal length
mirror produces a reduced, upright, virtual image.) The equation in the solution to Problem 5(a) can be used to find the object distance in terms off and the magnification, t? = f (1 - h/hf) = f (1 - 1/M) = -20 cm(1- 3) = 40 cm.
image appears on a screen located 31 cm on the
of the lens? (b) By how much is the image enlarged or reduced?
Solution (a) The object and image distances are both positive, for a real image formed by a single lens (recall that only a real image can appear on a screen), so the lens equation gives f-I = (56 cm)-' + (31 cm)-' = (20.0 cm)-'. (b) Equation 36-4 gives a magnification of M = -31156 = -0.554, so the inverted image is reduced to nearly 55% of the actual size of the bulb.
and solve for t'. The result is t?' = ef / ( t? - f ) = (80x45 cm)/(800 - 45) = 4.77 cm.
problem
27. A lens has focal length f = 35 cm. Find the type and height of the image produced when a 2.2-cm-high object is placed at distances (a) f + 10 cm and (b) f - 10 cm.
Solution The lens equation and magnification for a thin (converging, i.e., positive f ) lens, Equations 3 6 4 and 5, give M = -el/! = - f/(! - f), SO h1 = Mh = - j h + (P- f ). (a) I f f = 3 5 cm a n d e = j + 1 0 c m , then