The rapid change in the propagation direction of a wave that reaches the boundary between two mediums is known as reflection. At least a portion of the approaching wave disturbance is contained within the same medium.
The different types of reflection are as follows:
When comparing angles of reflection between spots on such uneven surfaces, the angle of reflection is completely random. When rays strike a rough surface at slightly different spots, they are reflected in completely opposite directions. This is known as diffused reflection and it is what allows us to perceive non-shiny objects.
3.Multiple reflection: When an object is placed in front of a mirror, it creates a single picture. When we use two mirrors, A single source of light can be reflected several times because reflective surfaces like mirrors are very good at retaining the intensity of light in a reflection. This multiple reflection is feasible until the light intensity is so low that we can no longer detect it. As a result, we can have an almost unlimited number of multiple reflections. Every unique reflection also reflects an image. This means that each image is a result of an image or another image.
The angle between the two mirrors has a big impact on the number of images we view. We can observe that as the angle between the mirrors is reduced, the number of pictures increases. The number of pictures reaches unlimited when the angle is zero, i.e., when the mirrors are parallel to each other.
A wavefront is the location of all points that are in the same phase. Wavefronts are of three types. They are as follows:
Huygen first proposed that light moves in waves in 1678. After escaping from the light source, these waves travel at the speed of light in all directions. Huygen proposed a straight forward geometrical method for calculating the propagation of a wavefront.
Let AB denote a segment of the wavefront at any given time ‘t’. To find the wavefront at any time
t + Δt, perform these steps:
According to the law of reflection:
Assume that AB is the plane wavefront incident on the plane mirror M1 M2 . Let ∠BAA’ = ∠i be the incident angle. The incident rays perpendicular to wavefront AB are 1, 2 and 3.
Every point on the wavefront AB, according to Huygens’ Principle, is a source of secondary wavelets. Assume secondary wavelets from point B arrive at location A’ in time t.
BA’ = c x t ……………………..(1)
c= velocity of light in vacuum
Assume secondary wavelets from point A arrive at point B’ in time t.
AB’ = c x t ………………………(2)
If you join A’ and B’, the reflected wavefront will be A’B’. The reflected rays perpendicular to A’B’ are 1′, 2′ and 3′. Also, let B’A’A = r be the reflection angle.
We have AA’B and AA’B’ from similar triangles.
BA’ = AB’ (From (1) and (2))
∠B = ∠B’ (Both are 90)
AA’ = AA’ (Common Base)
Hence, triangles are congruent.
∠i = ∠r
This is also known as Snell’s Law of reflection.
The phenomenon of light waves colliding with a surface and bouncing back is known as reflection. Huygens’ Principle is used to verify the laws of reflection. The incident ray, the reflected ray and normal to the surface at the point of incidence, all lie in the same plane. Angle of reflection equals angle of incidence. The Huygens Principle, proposed in 1690 by the Dutch mathematician, scientist and astronomer Christiaan Huygens, is a powerful tool for examining many optical phenomena.