Analyzing the Setup
Imagine you are looking at a beautifully coated piece of glass. We have a glass plate with a refractive index of 1.5, and on top of it sits a thin layer of a different material with a refractive index of 1.8. Light from the air (where the refractive index is 1) is shining directly down onto this setup.
When the light hits the first boundary (between the air and the thin layer), part of it reflects back up. We'll call this Ray 1. The rest of the light travels through the thin layer, hits the second boundary (between the thin layer and the glass), and reflects back up again. We'll call this Ray 2. These two reflected rays will eventually meet and interfere with each other. Our goal is to find the condition for them to interfere constructively, meaning they combine to form a bright spot.
The Master Equation
To understand how these rays interfere, we first need to look at the
optical path difference between them. Ray 2 travels an extra distance by going down through the thin layer of thickness
t and coming back up. Since it travels this distance inside a medium with a refractive index of
μ1=1.8, the optical path difference is:
Δx=2μ1t=2(1.8)t=3.6t
But wait, there is a catch here! We must also consider the phase changes that occur upon reflection.
When light reflects off a medium that is optically denser (has a higher refractive index), it undergoes a phase shift of π. Ray 1 reflects off the thin layer (μ1=1.8) while traveling in air (μ=1). Since 1.8>1, Ray 1 experiences a phase shift of π.
On the other hand, Ray 2 reflects off the glass (μ2=1.5) while traveling in the thin layer (μ1=1.8). Since 1.5<1.8, it is reflecting off a rarer medium, so it experiences no phase shift.
Because only one of the rays experiences a phase shift of
π, the two rays have an inherent phase difference of
π. For them to interfere constructively, the optical path difference must compensate for this by being an odd multiple of half the wavelength. Therefore, the condition for constructive interference is:
Δx=(n−21)λwhere n=1,2,3,…
Final Calculation
Now, let's substitute our optical path difference into the condition:
3.6t=(n−21)λ
We are asked to find the
least value of the thickness
t. To make
t as small as possible, we should choose the smallest valid integer for
n, which is
n=1. Substituting
n=1 gives:
3.6t=(1−21)λ=2λ
We are given that the wavelength of the light is
λ=648 nm. Let's plug that in and solve for
t:
t=2×3.6648
t=7.2648
t=90 nm
And there we have it! The minimum thickness of the layer required for constructive interference is 90 nm.