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50 through 57 55, 57 53 Thin lenses. Object Ostands on the central axis of a thin symmetric lens. For this situation, each problem in Table 34-6 gives object distance p (centimeters), the type of lens (C stands for converging and D for diverging), and then the distance (centimeters, without proper sign) between a focal point and the lens. Find (a) the image distance iand (b) the lateral magnification m of the object, including signs. Also, determine whether the image is (c) real (R) or virtual (V), (d) inverted (I) from object Oor non inverted (NI), and (e) on the same side of the lens as object Oor on the opposite side.

Short Answer

Expert verified
  1. Image distance i=-48cm
  2. Lateral magnification localid="1663064475861" m=+4.0
  3. Image is virtual V
  4. Image is non-inverted N

e. Image is on the same side of the object.

Step by step solution

01

Listing the given quantities

The lens is converging

Focal length,f=16.0cm

Object distance, p=+12cm

02

Understanding the concepts of lens equation and the formula for magnification

By using the thin lens equation and the formula for magnification, we can find all the required quantities.

Formula:

Thin lens equation, 1f=1p+1i

Magnification, m=-ip

03

(a) Calculations of the image distance

Since the lens is converging, the focal length value should be positive, i.e.

f=+16.0cm

Thin lens equation is

1f=1p+1i116=112+1i1i=116-1121i=-0.021i=-47.61≈-48cm

Image distance =-48cm

04

(b) Calculations of the magnification

Magnification is,

m=ipm=--48.012m=+4.0cm

Lateral magnification m=+4.0

05

(c) Explanation

As the image distance iis negative, the image is virtualV.

06

(d) Explanation

As the magnification is positive, the image is non-inverted NI.

07

(e) Explanation

For thin lens, the real images forms on the opposite side as the object and virtual images form on the same side as the object.

Since the image is non-inverted, it forms on the same side of the object.

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Most popular questions from this chapter

Figure 34-56 shows a beam expander made with two coaxial converging lenses of focal lengths f1and f1and separationd=f1+f2. The device can expand a laser beam while keeping the light rays in the beam parallel to the central axis through the lenses. Suppose a uniform laser beam of width Wi=2.5mmand intensity Ii=9.0kW/m2enters a beam expander for whichf1=12.5cmand f2=30.0cm.What are (a) Wfand (b) lfof the beam leaving the expander? (c) What value of d is needed for the beam expander if lens 1 is replaced with a diverging lens of focal lengthf1=-26.0cm?

50 through 57 55, 57 53 Thin lenses. Object Ostands on the central axis of a thin symmetric lens. For this situation, each problem in Table 34-6 gives object distance p (centimeters), the type of lens (C stands for converging and D for diverging), and then the distance (centimeters, without proper sign) between a focal point and the lens. Find (a) the image distance i and (b) the lateral magnification m of the object, including signs. Also, determine whether the image is (c) real (R) or virtual (V) , (d) inverted (I) from object or non-inverted (NI) , and (e) on the same side of the lens as object Oor on the opposite side.

The equation 1p+1i=2rfor spherical mirrors is an approximation that is valid if the image is formed by rays that make only small angles with the central axis. In reality, many of the angles are large, which smears the image a little. You can determine how much. Refer to Fig. 34-22 and consider a ray that leaves a point source (the object) on the central axis and that makes an angle a with that axis. First, find the point of intersection of the ray with the mirror. If the coordinates of this intersection point are x and y and the origin is placed at the center of curvature, then y=(x+p-r)tan a and x2+ y2= r2where pis the object distance and r is the mirror’s radius of curvature. Next, use tanβ=yxto find the angle b at the point of intersection, and then useα+y=2βtofind the value of g. Finally, use the relationtany=y(x+i-r)to find the distance iof the image. (a) Suppose r=12cmand r=12cm. For each of the following values of a, find the position of the image — that is, the position of the point where the reflected ray crosses the central axis:(0.500,0.100,0.0100rad). Compare the results with those obtained with theequation1p+1i=2r.(b) Repeat the calculations for p=4.00cm.

Figure 34-25 shows a fish and a fish stalker in water. (a) Does the stalker see the fish in the general region of point a or point b? (b) Does the fish see the (wild) eyes of the stalker in the general region of point c or point d?

Figure 34-46a shows the basic structure of an old film camera. A lens can be moved forward or back to produce an image on film at the back of the camera. For a certain camera, with the distance i between the lens and the film set at f = 5.00 cm, parallel light rays from a very distant object O converge to a point image on the film, as shown. The object is now brought closer, to a distance of p = 100 cm, and the lens–film distance is adjusted so that an inverted real image forms on the film (Fig. 34-46b). (a) What is the lens–film distance i now? (b) By how much was distance i changed?

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