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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?

Short Answer

Expert verified
  1. If a point image is produced at the back of the sphere, the refractive index of the sphere is 2.00.
  2. It is not possible to produce a point image at the center of the sphere.

Step by step solution

01

Step 1: Given data

  • The object distance isp=
  • Refractive index;n1=nair=1
02

Determining the concept

Using the relation between the index of refraction of object and image, image distance, object distance, and the radius of curvature, given by equation 34-8, find the required answers.

Formulae are as follows:

n1p+n2i=n2-n1r

Here, p is the pole, i is the image distance.

03

(a) Determining the refractive index of the sphere, if a point image is produced at the back of the sphere.

As the image is produced at the back of the sphere, so,

i = 2r

n1p+n2i=n2-n1r

Substituting the given values,

1+n22r=n2-1r

n22r=n2-1rn22=n2-1n21-12=1n22=1n2=2.00

Hence, if a point image is produced at the back of the sphere, the refractive index of the sphere is 2.00.

04

(b) Determine the refractive index of the sphere that will produce a point image at the center of the sphere.

For an image to be produced at the center of the sphere,

i=rn1p+n2i=n2-n1r

Substituting the given values,

role="math" localid="1662977840109" n1+n2r=n2-1rn2r=n2-1r

This is not valid unless n2or r

Hence, it is impossible to produce a point image at the center of the sphere.

The required quantities can be found by using the relation between the index of refraction of object and image, the image distance, the object distance, and the radius of curvature.

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Most popular questions from this chapter

The formula 1p+1i=1f is called the Gaussian form of the thin-lens formula. Another form of this formula, the Newtonian form, is obtained by considering the distance xfrom the object to the first focal point and the distancex' from the second focal point to the image. Show thatxx'=f2 is the Newtonian form of the thin-lens formula

A point object is 10cmaway from a plane mirror, and the eye of an observer (with pupil diameter5.0mm) is 20cmaway. Assuming the eye and the object to be on the same line perpendicular to the mirror surface, find the area of the mirror used in observing the reflection of the point.

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 p, index of refraction n of the lens, radius r1of the nearer lens surface, and radius localid="1663061304344" r2of the farther lens surface. (All distances are in centimeters.) Find (a) the image distance iand (b) the lateral magnification mof the object, including signs. Also, determine whether the image is (c) real (R)or virtual (V),(d) inverted (I)from the object Oor non-inverted (NI), and (e) on the same side of the lens as object Oor on the opposite side.

58 through 67 61 59 Lenses with given radii. Object stands 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 of the nearer lens surface, and radius of the farther lens surface. (All distances are in centimetres.) Find (a) the image distance and (b) the lateral magnification m of the object, including signs. Also, determine whether the image is (c) real (R) or virtual , (d) inverted from object or non-inverted (NI), and (e) on the same side of the lens as object or on the opposite side

Figure 34-47a shows the basic structure of the human eye. Light refracts into the eye through the cornea and is then further redirected by a lens whose shape (and thus ability to focus the light) is controlled by muscles. We can treat the cornea and eye lens as a single effective thin lens (Fig. 34-47b). A 鈥渘ormal鈥 eye can focus parallel light rays from a distant object O to a point on the retina at the back of the eye, where the processing of the visual information begins. As an object is brought close to the eye, however, the muscles must change the shape of the lens so that rays form an inverted real image on the retina (Fig. 34-47c). (a) Suppose that for the parallel rays of Figs. 34-47a and b, the focal length fof the effective thin lens of the eye is 2.50 cm. For an object at distance p = 40 cm, what focal length f of the effective lens is required for the object to be seen clearly? (b) Must the eye muscles increase or decrease the radii of curvature of the eye lens to give focal length f?

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