In Fig. 34-26, stick figure O stands in front of a thin, symmetric lens that is mounted within the boxed region; the central axis through the lens is shown. The four stick figuresI1andI4suggest general locations and orientations for the images that might be produced by the lens. (The figures are only sketched in; neither their height nor their distance from the lens is drawn to scale.) (a) Which of the stick figures could not possibly represent images? Of the possible images, (b) which would be due to a converging lens, (c) which would be due to a diverging lens, (d) which would be virtual, and (e) which would involve negative magnification?

Short Answer

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(a) The sick figures that could not possibly represent images areI2andI3.

(b) The sick figures that represent a converging lens areI1andI4.

(c) The sick figure that represents a diverging lens isI1.

(d) The sick figure that represents a virtual magnification isI1.

(e)The sick figure that represents a negative magnification is I4.

Step by step solution

01

Definition of a converging lens and diverging lens

The lens that allows the rays of light to focus on one point is termed a converging lens and the lens that allows the rays of light from one point to scatter at different points is termed a diverging lens.

02

(a) Determination of the sick figures that could not possibly represent images

The lens forms an image on the left of the lens as upright and on the right of the lens as inverted.

Thus, the sick figures that could not possibly represent images are I2andI3.

03

(b) Determination of the sick figures that represent a converging lens

The converging lens forms an image on the left of the lens as upright and on the right of the lens as inverted.

Thus, the sick figures that represent a converging lens are I1andI4.

04

(c) Determination of the sick figures that represent a diverging lens

The image due to a diverging lens is always virtual and is located between the object and the lens.

Thus, the sick figure that represents a diverging lens is I1.

05

(d) Determination of the sick figure that represents a virtual magnification

From the figure, it can be observed that I1is a virtual image due to the lens.

Thus, the sick figure that represents a virtual magnification is I1.

06

(e) Determination of the sick figure that represents a negative magnification

It is known that when the image is inverted, there would be a negative magnification.

Thus, the sick figure that represents a negative magnification is I4.

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Most popular questions from this chapter

You produce an image of the Sun on a screen, using a thin lens whose focal length is 20cm. What is the diameter of the image? (See Appendix C for needed data on the Sun.)

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 O or non inverted (NI) , and (e) on the same side of the lens as object Oor on the opposite side.

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 moth at about eye level is10cmin front of a plane mirror; a man is behind the moth,30cmfrom the mirror. What is the distance between man’s eyes and the apparent position of the moth’s image in the mirror?

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 “normal” 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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