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


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?

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.

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?

(a) Show that if the object O in Fig. 34-19c is moved from focal point F1toward the observer’s eye, the image moves in from infinity and the angle (and thus the angular magnification mu) increases. (b) If you continue this process, where is the image when mu has its maximum usable value? (You can then still increase, but the image will no longer be clear.) (c) Show that the maximum usable value of ismθ=1+25cmf.(d) Show that in this situation the angular magnification is equal to the lateral magnification.

An object is placed against the center of a spherical mirror and then moved 70 cm from it along the central axis as the image distance i is measured. Figure 34-48 gives i versus object distance p out to ps=40cm. What is the image distance when the object is 70 cm from the mirror?

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