** ****Behaviour of li****ght !!**

Light is an electromagnetic wave and during its propagation it encounters various types of obstacles. There are circumstances where this type of wave behaves to a good approximation as if they travel in straight line. For this, it is necessary that the obstacles have dimensions much greater than wavelength of light. This special case of wave behaviour is considered in geometrical optics.

For dealing with geometrical or ray optics it has to be defined that what is the essence of this particular subject. To study this the first need is to define a ray.

** Ray!!**

A ray is defined to be the line along which light propagates. It is the normal to all the wavefronts of that particular disturbance. Since it defines the direction of propagation the formation of images or distraction by another medium can be better explained because the process of reflection, refraction etc. can be visualised in a better way. The main principle governing the whole of ray optics is Fermat’s principle which says that in going from one medium to another, the path followed by a light ray is that for which the time taken is either minimum or maximum.

**Definition :**

We know that a ray of light is composed of packets of energy known as photons. The photons have the ability of colliding with any surface.

Thus the photons transfer momentum & energy in the same way as the transfer of momentum & energy take place between any two particles during collision.

For elastic collision a particle gets rebounded with same speed where as the direction of its motion changes due to the impact (impulsive) force offered by the other colliding particle.

Similarly when a photon is incident on a fine plane surface, it gets rebounded. This is known as R**eflection**.

**What are the laws of reflection ?**

There are two laws governing the physical phenomenon of reflection.

They are-

(i) The incident ray, normal to the interface and the reflected ray lie on the same plane.

(ii) The angle of incidence is equal to the angle of reflection.

We can observe from the figure that two rays coming from a point object O are reflected at the points M & N. If the reflected rays are produced back they meet at a point P. This point P is known as image.

Since the image is formed at the back of the mirror, it is known as virtual image .

Geometrically we can see that object distance is equal to image distance from mirror surface p = q

(As ΔOMP & ΔONP are isosceles triangles)

__Properties of image formed by plane m__

Properties of image formed by plane mirror

(a) the image is virtual erect and laterally reversed.

(b) the image size = object size

(c) object distance = image distance

(d) when the plane mirror is rotated through an angle θ,

the reflected ray is rotated through an angle 2θ.

(e) the numbers of images formed by the combination of two mirrors inclined at an angle θ,

Where [ ] represents the greatest integer

**e.g.** When two plane mirrors are placed parallel to each other ,

then θ = 0

⇒ N = ∞

Therefore infinite number of images are formed.

**Example :** If an object moves towards a plane mirror with a speed V at an angle θ to the perpendicular to the plane of the mirror, find the relative velocity between the object & the image.

**Solution :**

Velocity of the object relative to the image is given as

**Exercise 1:** Prove that if the plane mirror rotates through an angle θ, the reflected ray for any incident ray is deviated through an angle 2θ.

**Example :** Find the minimum length of the mirror required to visualise the complete image of the body of a person of height H.

**Solution:** The person must have to obtain a reflected ray one from his head & another reflected ray from the feet.

Geometrically, AC = AB + BC where

AB = x/2 and BC = (H−x)/2

AC = x/2 + (H−x)/2

AC = H/2

i.e. length of the mirror is just half the height of person.

*Illustration:*

Show that if a mirror is rotated by angle θ the reflected ray rotates through an angle 2θ When the mirror rotates by θ , the angle between the normals is also equal to θ.

**Solution :**

Incidence angle for M’ = i + θ

Angle of reflection for M’ = i + θ

i.e. ∠N_{2}OR_{2} = i + θ

∠N_{1}OR_{2} = ∠N_{1}ON_{2} + ∠N_{2}OR_{2}

= θ + i + θ = i + 2 θ

or ∠R_{1}OR_{2} = ∠N_{2}OR_{2} -∠N_{2}OR_{1}

= i + 2 θ – i = 2 θ

Hence the reflected ray rotates by an angle 2θ

**Exercise 2:** Find the number of images formed when two plane mirrors are placed at right angle to each other & locate the images by drawing ray diagram.

**Exercise 3:** Draw the ray diagram for the images formed by an object placed in between two plane parallel mirrors due to both the reflecting surfaces