58 through 67 61 59 Lenses with given radii. An object Ostands in front of a thin lens, on the central axis. For this situation, each problem in Table 34-7 gives object distance , index of refraction n of the lens, radius localid="1662989860522" r1of the nearer lens surface, and radius localid="1662988669866" r2of the farther lens surface. (All distances are in centimeters.) Find (a) the image distance iand (b) the lateral magnification m of the object, including signs. Also, determine whether the image is (c) real localid="1662988718474" Ror virtual localid="1662988727007" V, (d) inverted localid="1662988740117" Ifrom object or non-inverted localid="1662989876683" NI, and (e) on the same side of the lens as objectOor on the opposite side.

Short Answer

Expert verified
  1. The image distance is-18cm .
  2. The lateral magnification of the object is+0.76$ .
  3. The image is virtual V.
  4. The image is not inverted Nlfrom object.
  5. The image on the same side of the object.

Step by step solution

01

The given data

  1. The object distance,P=+24cm
  2. The index of refraction of the lens, n=150
  3. The radius of the nearer lens surface,r1=-15mm
  4. The radius of the farther lens surface,r2=-25mm
02

Understanding the concept of properties of the lens

We can use the concept of the lens formula and lens marker’s equation. The focal length of the lens is positive for a converging lens and negative for a diverging lens. The diverging lens can form a virtual image. If the object is outside the focal point, then it is a real image and if the object is inside the focal point, then it is a virtual image.

Formula:

The lens formula for refraction, 1f=n-11r1-1r2 (i)

The lens formula, 1f=1P¯+1i (ii)

The magnification formula of the lens, m=ii (iii)

03

(a) Calculation of the object distance

Using the given data in equation (i), the expression of the focal length of the lens in air is given as follows:

f=r1r2n-1r2-r1=-15cm-25cm1.50-1-25cm--15cm=-75cm

The given lens is a diverging lens because focal length is negative.

For an object in front of the lens, the object distance and image distance are related to the lens’ focal length. Thus, the image distance can be given using the data in equation (ii) as follows:

1i=1f-1Pi=PfP-f=+24cm-75cm+24cm--75cm=-18cm

Hence, the value of the image distance is .

04

(b) Calculation of the lateral magnification of the object

The lateral magnification is the ratio of the object distance to the image distance . It is given using the data in equation (iii) as follows:

m=--18cm+24cm=+0.76

Hence, the value of the lateral magnification is +0.76$ .

05

(c) Calculation of the behavior of the image

If the object is inside the focal point, then it is a virtual image.The image distance is also negative.

Hence, the image is virtual

06

(d) Calculation if the image is inverted or not

The value of magnification is positive.

Hence, the image is not inverted .

07

(e) Calculation of the position of the image

The image distance is negative.

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

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Most popular questions from this chapter

80 through 87 80, 87 SSM WWW 83 Two-lens systems. In Fig. 34-45, stick figure O (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 O, 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 C for converging and D for diverging; the number after C or D 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 O or non- inverted (NI), and (e) on the same side of lens 2 as object O or on the opposite side.

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?

A pepper seed is placed in front of a lens. The lateral magnification of the seed is +0.300. The absolute value of the lens’s focal length is40.0cm. How far from the lens is the image?

In a microscope of the type shown in Fig. 34-20, the focal length of the objective is 4.00 cm, and that of the eyepiece is 8.00 cm. The distance between the lenses is 25.00 cm. (a) What is the tube length s? (b) If image I in Fig. 34-20 is to be just inside focal point F1, how far from the objective should the object be? What then are (c) the lateral magnification m of the objective, (d) the angular magnification mθ of the eyepiece, and (e) the overall magnification M of the microscope?


Isaac Newton, having convinced himself (erroneously as it turned out) that chromatic aberration is an inherent property of refracting telescopes, invented the reflecting telescope, shown schematically in Fig. 34-59. He presented his second model of this telescope, with a magnifying power of 38, to the Royal Society (of London), which still has it. In Fig. 34-59, incident light falls, closely parallel to the telescope axis, on the objective mirror. After reflection from the small mirror (the figure is not to scale), the rays form a real, inverted image in the focal plane (the plane perpendicular to the line of sight, at focal point F). This image is then viewed through an eyepiece. (a) Show that the angular magnification for the device is given by Eq. 34-15:

mθ=fob/fey

fob

the focal length of the objective is a mirror and

feyis that of the eyepiece.

(b) The 200 in. mirror in the reflecting telescope at Mt. Palomar in California has a focal length of 16.8 m. Estimate the size of the image formed by this mirror when the object is a meter stick 2.0 km away. Assume parallel incident rays. (c) The mirror of a different reflecting astronomical telescope has an effective radius of curvature of 10 m (“effective” because such mirrors are ground to a parabolic rather than a spherical shape, to eliminate spherical aberration defects). To give an angular magnification of 200, what must be the focal length of the eyepiece?

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