In Fig. 34-32, an isotropic point source of light Sis positioned at distancedfrom a viewing screen Aand the light intensityIPat pointP(level withS) is measured. Then a plane mirrorMis placed behindSat distanced. By how much isIPmultiplied by the presence of the mirror?

Short Answer

Expert verified

The light intensity Ipis multiplied by 1.11.

Step by step solution

01

Identification of the given data

The given data is listed as follows,

  • Distance between the source and the pointPisd.
  • The intensity of the light at point is IP.
02

Expression of the intensity due to source

The intensity due to the sourceSis expressed as follows,

Ip=Ad2 …(i)

Here, Ais the constant, and dis the distance between the source and the point.

The total intensity due to the presence of the mirror will be the sum of the intensity due to the source and the intensity due to the image.

03

Determination of the amount of the light intensity that is multiplied by the presence of the mirror

Now, if the plane mirror is placed behindSat a distanced, then the image will be formed at a distancedbehind the mirror. So, the total distance from the image to the pointPis as follows,

d'=3d

The intensity due to the image is as follows,

I'=A3d2=A9d2

…(ii)

It can be observed from equations (i) and (ii),

I'=Ip9

The total intensity at point Pdue to the presence of the mirror will be the sum of the intensity due to the source, and the intensity due to the image.

I=Ip+I'=Ip+Ip9=10Ip9=1.11Ip

Thus, the light intensity Ipis multiplied by 1.11.

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Most popular questions from this chapter

(a) A luminous point is moving at speedV0toward a spherical mirror with a radius of curvaturer, along the central axis of the mirror. Show that the image of this point is moving at the speed

vI=-(r2p-r)2v0

Where,p is the distance of the luminous point from the mirror at any given time. Now assume the mirror is concave, withr=15cm.and letV0=5cm/s. FindV1when (b)p=30cm(far outside the focal point), (c) p=8.0cm(just outside the focal point), and (d)p=10mm(very near the mirror).

(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.

A millipede sits 1.0min front of the nearest part of the surface of a shiny sphere of diameter 0.70m(a) How far from the surface does the millipede’s image appear? (b) If the millipede’s height is 2.0mm, what is the image height? (c) Is the image inverted?

Figure 34-37 gives the lateral magnification mof an object versus the object distanc pfrom a spherical mirror as the object is moved along the mirror’s central axis through a range of values p. The horizontal scale is set by Ps=10.0mm. What is the magnification of the object when the object is 21cm from the mirror?

Prove that if a plane mirror is rotated through an angle a, the reflected beam is rotated through an angle 2α. Show that this result is reasonable for α=45∘.

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