Class 12 Physics Nature and propagation of Light Notes

UNIT 3
CLASS 12 PHYSICS • WAVE AND OPTICS

Nature and Propagation of Light

Chapter 10

Wave Front and Wavelet

According to wave theory of light, source of light sends out wave in all direction in the form of disturbance.

Wave front is defined as locus of all points equi-distance from source of light which are vibrating in same phase.

Each point on wave front can act like a new source of small spherical wave which are called wavelets.

Wave front with secondary wavelets produced by points on the wave front Source Wave front Wavelet
Wave front and secondary wavelets

Types of Wave Front

Depending upon the shape of source of light, wave front is of three types:

1. Spherical Wave Front

Wave front produced by point source of light is called spherical wave front.

2. Cylindrical Wave Front

Wave front produced by linear source of light is called cylindrical wave front.

3. Plane Wave Front

A small part of spherical or cylindrical wave front, or a wave front from a distant source, forms a wave front in the form of plane and is called plane wave front.
Spherical, cylindrical and plane wave fronts Spherical wave front Point source Cylindrical wave front Linear source Plane wave front Distant source
Three types of wave front

Huygens’ Principle

It states that:

  1. Each point on a given wave front acts as a new source of disturbance which propagates in all direction with a velocity equal to velocity of light.
  2. The tangential surface touching the secondary wavelets in forward direction at any instant gives a new wave front called secondary wave front.

Construction of Secondary Wave Front

Huygens construction showing a primary wave front, secondary wavelets and the new secondary wave front Source Primary wave front AB Secondary wave front A′B′ Forward direction Secondary wavelets
Fig: Huygens’ principle

Suppose AB be a section of given wave front called primary wave front at any instant. Let a, b, c and d be points on this wave front. The distance travelled by light in time t is equal to ct.

At each point as a centre, if spheres of radius ct are constructed, the spherical surfaces represent positions of secondary wavelets. The tangential surface touching these spheres in forward direction represents secondary wave front.

Law of Reflection on the Basis of Wave Theory

The laws of reflection are:

1. The angle of reflection ‘r’ is equal to angle of incidence ‘i’ for all wavelength and for any pair of medium.
∠i = ∠r
2. The incident ray, the reflected ray and the normal to the reflecting surface all lie on the same plane.

To Prove Law of Reflection on the Basis of Wave Theory

Huygens construction for reflection of a plane wave front at a plane surface Reflecting surface XY Incident wave front AB Reflected wave front A′B′ i r Normal
Reflection at a plane surface using Huygens’ principle

Consider a plane wave front AB incident on reflecting surface XY at an angle of incidence ‘i’. Let the incident rays be perpendicular to wave front AB and AN be normal to reflecting surface.

Let in time ‘t’ one point of wave front reach the reflecting surface. At the same time, secondary wavelet from the point already on the reflecting surface spreads out in the form of sphere of radius ct.

Distance travelled by light in same time = ct
Therefore corresponding sides in the construction are equal.
The two right-angled triangles formed by the incident and reflected wave fronts are congruent.
∠i = ∠r

Therefore, the angle of incidence is equal to the angle of reflection, which is the first law of reflection of light.

Further, the incident wave front, reflecting wave front and reflecting surface are perpendicular to the plane of paper. So incident ray, reflected ray and normal lie in the same plane.

Law of Refraction on the Basis of Wave Theory

The refraction laws are:

1. The ratio of sine of angle of incidence to the sine of angle of refraction is constant for any two given medium.
μ = sin i / sin r
where μ = refractive index of medium
2. The incident ray, the refracted ray and the normal at the point of incidence lie on same plane.

To Prove Law of Refraction on the Basis of Wave Theory

Huygens construction for refraction of a plane wave front at a plane boundary between rarer and denser media Rarer medium Denser medium Surface XY Incident wave front AB Refracted wave front A′B′ i r
Refraction at a plane surface using Huygens’ principle

Consider a plane wave front AB incident on plane surface XY separating two media. The rays perpendicular to wave front AB represent incident rays and AN is normal to surface XY.

Let v and c be the velocity of light in denser and rarer medium respectively. According to Huygens’ theory, every point on AB acts as source of secondary wavelet.

Let ‘t’ be the time taken by light to reach the next point on the boundary in the rarer medium. Then:

BA′ = ct
Secondary wavelet originating from A in denser medium travels distance:
AB′ = vt

From the geometry of the two right triangles:

sin i = BA′/AA′
sin r = AB′/AA′

Therefore:

sin i / sin r = BA′/AB′
= ct/vt
= c/v
sin i / sin r = μ

which proves first law of refraction.

Further, the incident wave front AB, refracting wave front A′B′ and refracting surface are perpendicular to the plane of paper. Hence incident ray, refracted ray and normal all lie on same plane.

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