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95 through 100. Three-lens systems. In Fig. 34-49, stick figure O (the object) stands on the common central axis of three thin, symmetric lenses, which are mounted in the boxed regions. Lens 1 is mounted within the boxed region closest to O, which is at object distance p1. Lens 2 is mounted within the middle boxed region, at distance d12from lens 1. Lens 3 is mounted in the farthest boxed region, at distance d23from lens 2. Each problem in Table 34-10 refers to a different combination of lenses and different values for distances, which are given in centimeters. The type of lens is indicated by C for converging and D for diverging; the number after C or D is the distance between a lens and either of the focal points (the proper sign of the focal distance is not indicated). Find (a) the image distance i3 \for the (final) image produced by lens 3 (the final image produced by the system) and (b) the overall lateral magnification M for the system, including signs. Also, determine whether the final image is (c) real (R)or virtual (V) , (d) inverted (I) from object O or non-inverted (Nl), and (e) on the same side of lens 3 as object O or on the opposite side.

Short Answer

Expert verified
  1. The image distance due to the image produced by lens 3 is i3=-5.2cm.
  2. The overall lateral magnification is m=+0.29.
  3. The final image is virtual.i3=-5.2cm
  4. The final image is non-inverted.
  5. The final image is on the same side of the object.

Step by step solution

01

Given data

  • Focal length

f1=6.0cm

f2=4.0cm

width="87" height="25" role="math">f3=12.0cm

  • Objects distance; p1=4.0cm
  • Distance between the lens 1 and 2; d12=8.0cm
  • Distance between the lens 2 and 3; d23=5.7cm
02

: Determining the concept

First, find out the image distance for each lens using the lens formula. After that, find the magnification of each lens using the corresponding formula. Using this, find the total magnification. From the sign of the total magnification, conclude whether the image is inverted or non-inverted. Also from the sign of the final image distance for the last lens, conclude whether the image is real or virtual and on which side of the object the final image is present.

Formulae are as follows:

1f=1p+1i

Here, mis the magnification, pis the pole, fis the focal length, and iis the image distance.

03

(a) Determining the image distance  i3 due to the image produced by the lens 3

According to the equation 34-4, first, find the image distance i1 as
1f=1p+1i

The lens 1 is converging, so the focal length of the length is positive.

1f1=1p1+1i1

1i1=1f1-1p1

So,

i1=f1p1p1-f1

Substituting the value,

i1=4ร—64-6=-242=-12.0cm

So now find thep2i.e., the object distance due to the second lens.

role="math" localid="1663216199144" p2=d12-i1

Putting the value ofp2=8.0--12.0

p2=20.0cm

From p2 calculate the image distancei2produced by the lens 2:

1f2=1p2+1i2

Here, lens 2 is diverging, so the focal length is negative.

1i2=1f2-1p2

So,

i2=f2p2p2-f2

Substituting the value,

i2=20.0ร—-420+4=-8024=-3.33cm

Now calculate the object distance p3as,

p3=d23-i2

Putting the value ofi2,

p3=5.7--3.33=9.3cm

Now calculate the image distance due to the lens 3 as,

1f3=1p3+1i3

Lens three is the diverging lens, so the focal length is negative so that,

1i3=1f3-1p3

So,

i3=f3p3p3-f3

Substituting the value,

i3=9.3ร—-12.09.3--12.0=-111.621.3=-5.23

So,

i3โ‰ˆ-5.2cm

Therefore, the image distance i3 due to the image produced by the lens 3 is i3=-5.2cm.

04

(b) Determine the overall lateral magnification

Now calculate the lateral magnification. The total magnification is the product of the magnification due to each lens.

m=-ip

Magnification for the lens 1;

m1=-i1p1

Substituting the values,

m1=--12.04=3.0m1=--12.04=3.0

Magnification for the lens 2;

m2=-i2p2

Substituting the values,

m2=--3.3320.0=0.17

Magnification for the lens 3;

m3=-i3p3

Substituting the values,

m3=--5.29.3=0.56

So, the total magnification is,

m=m1m2m3

Substitute the above calculated values of the magnification;

m=3ร—0.17ร—0.56=0.285โ‰ˆ+0.29

Therefore, the overall lateral magnification is m=+0.29.

05

(c) Determine whether the final image is real or virtual

If the image distance fromthelast lens is positive, then the image is real, and if the image distance due tothelast lens is negative, then the image is virtual.

In this casei3is negative, so the image is virtual.

Therefore, the final image is virtual.

06

(d) Determine whether the final image is inverted or non-inverted

If the total magnification is positive, then the image is non-inverted, and if the total magnification is negative, then the image is inverted.

In our case, the total magnification is positive.

Hence, the image is non-inverted.

07

(e) Determine whether the final image is on the same side or opposite side of the object

The result c), concludes that the image is virtual. So, the image is on the same side of lens 3 from the object.

Therefore, the final image is on the same side of the object.

The image distance for any lens and overall magnification of a three-lens system can be found using the corresponding formulae. The nature of the image can be predicted from the characteristics of the image formed due to the given three-lens system.

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Most popular questions from this chapter

An object is placed against the center of a thin lens and then moved away from it along the central axis as the image distance is measured. Figure 34-41 gives i versus object distance p out to ps=60cm. What is the image distancewhen p=100cm?

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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?

Suppose the farthest distance a person can see without visual aid is50cm. (a) What is the focal length of the corrective lens that will allow the person to see very far away? (b) Is the lens converging or diverging? (c) The power Pof a lens (in diopters) is equal to1/f, wherefis in meters. What ispfor the lens?

You grind the lenses shown in Fig. 34-53 from flat glass disks (n=1.5)using a machine that can grind a radius of curvature of either 40cmor 60cm. In a lens where either radius is appropriate, you select the 40cmradius. Then you hold each lens in sunshine to form an image of the Sun. What are the (a) focal length fand (b) image type (real or virtual) for (bi-convex) lens 1, (c)f and (d) image type for (plane-convex) lens 2, (e) f and (f) image type for (meniscus convex) lens 3, (g) f and (h) image type for (bi-concave) lens 4, (i) fand (j) image type for (plane-concave) lens 5, and (k) f and (l) image type for (meniscus concave) lens 6?

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