80 through 87 80, 87 SSM WWW 83 Two-lens systems. In Fig. 34-45, stick figure (the object) stands on the common central axis of two thin, symmetric lenses, which are mounted in the boxed regions. Lens 1 is mounted within the boxed region closer to, which is at object distance p1. Lens 2 is mounted within the farther boxed region, at distance d. Each problem in Table 34-9 refers to a different combination of lenses and different values for distances, which are given in centimeters. The type of lens is indicated by converging and for diverging; the number after or is the distance between a lens and either of its focal points (the proper sign of the focal distance is not indicated). Find (a) the image distance i2for the image produced by lens 2 (the final image produced by the system) and (b) the overall lateral magnification Mfor the system, including signs. Also, determine whether the final image is (c) real (R)or virtual (V), (d) inverted(I) from object or non-inverted (NI), and (e) on the same side of lens 2 as the object or on the opposite side.

Short Answer

Expert verified

a. Image distance for the image produced by lens 2,i2=+3.13cm

b. Overall lateral magnification, including sign,M=-0.31

The final image is,

c. Real (R)

d. Inverted (I)

e. On the opposite side from the object.

Step by step solution

01

Step 1: Given Information

The object stands on the common central axis of two thin symmetric lenses.

Distance between object and lenses 1,p1=+20cm

Distance between lens 1 and 2,d=8cm

Lens 1 is converging, focal lengthf1=9cm

Lens 2 is converging, focal lengthf2=5cm

02

Determining the concept

Using the relation between focal length, image distance and object distance find the image distance i2. Then using the formula for overall magnification find its value.

From the solution of part a and b answer part c, d and e.

Formula for focal length,1f=1p+1i

Overall magnification,M=m1m2

Magnification,m=-ip

Where,mis the magnification, pis the pole,fis the focal length, andiis the image distance.

03

 Determining the image distance for the image produced by lens 2,

(a)

For lens 1 focal length f1, object distancep1

Using the expression for focal length,

1f1=1p1+1i11i1=1f1-1p11i1=p1-f1f1p1i1=f1p1p1-f1

i1=f1p1p1-f1...1

i1=9×2020-9i1=18011i1=16.363~16.4cm.

This serves as an object for lens 2,p2=d-i1=8-16.4=-8.4cmand it is given thatf2=5cm

Modifying equation 1 for lens 2,

i2=f2p2p2-f2i2=5×-8.4-8.4-5i2=3.13cm

Therefore, the image produced by lens 2 is at 3.13cm.

04

Determining the overall lateral magnification, including sign, M

(b)

To find overall magnification use the formula,

M=m1m2

Magnification m=-ip

role="math" localid="1663056146339" M=-i1p1×-i2p2M=-16.420×-3.13-8.4M=-0.31

Therefore, the overall magnification for the given lens system is-0.31.

05

Determining whether the final image is real (R) or virtual (V).

(c)

Since the lens 1 and 2 are converging, the object for lens 2 is outside the focal point. The final image distance is positive.

Hence, the image formed by this lens system is real.

06

Determining whether the final image is inverted (I) or non-inverted (NI).

(d)

Overall magnification for this lens system is negative which shows that the image and the object have the opposite orientation.

Hence, the image is inverted.

07

Determining whether the final image is on the same side of lens 2 as object or on the opposite side.

(e)

The final image distance is positive, which shows that it is the positive side of lens 2 that is on the opposite side of the object.

Hence, the image is on the opposite side of the object.

The focal length and overall magnification of the two-lens system can be found using the corresponding formula. The nature of the image can be predicted from the characteristics of the image formed due to the given two-lens system.

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Most popular questions from this chapter

32 through 38 37, 38 33, 35 Spherical refracting surfaces. An object Ostandson the central axis of a spherical refracting surface. For this situation, each problem in Table 34-5 refers to the index of refractionn1where the objectis located, (a) the index of refraction n2on the other side of the refracting surface, (b) the object distance p, (c) the radius of curvature rof the surface, and (d) the image distance i. (All distances are in centimeters.) Fill in the missing information, including whether the image is (e) real (R)or virtual (V)and (f) on the same side of the surface asthe object Oor on the opposite side.

In Fig. 34-38, a beam of parallel light rays from a laser is incident on a solid transparent sphere of an index of refraction n. (a) If a point image is produced at the back of the sphere, what is the index of refraction of the sphere? (b) What index of refraction, if any, will produce a point image at the center of the sphere?

Figure 34-50a is an overhead view of two vertical plane mirrors with an object O placed between them. If you look into the mirrors, you see multiple images of O. You can find them by drawing the reflection in each mirror of the angular region between the mirrors, as is done in Fig. 34-50b for the left-hand mirror. Then draw the reflection of the reflection. Continue this on the left and on the right until the reflections meet or overlap at the rear of the mirrors. Then you can count the number of images of O. How many images of O would you see if θis (a) 90°, (b) 45°, and (c) 60°? If θ=120°, determine the (d) smallest and (e) largest number of images that can be seen, depending on your perspective and the location of O. (f) In each situation, draw the image locations and orientations as in Fig. 34-50b.

A short straight object of lengthLlies along the central axis of a spherical mirror, a distance pfrom the mirror. (a) Show that its image in the mirror has alength, L'=L(f/(p-f))2(Hint: Locate the two ends of the object.) (b) Show that the longitudinal magnification is equal tom'=(L'/L) is equal to m2, where m is the lateral magnification.

You look down at a coin that lies at the bottom of a pool of liquid of depthand index of refraction(Fig. 34-57). Because you view with two eyes, which intercept different rays of light from the coin, you perceive the coin to bewhere extensions of the intercepted rays cross, at depthdainstead of d. Assuming that the intercepted rays in Fig. 34-57 are close to a vertical axis through the coin, show that da=dn.


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