The pattern of diffraction of light in the single-slit experiment is different from those formed by double slits.
When we examine light waves, we learn about their many features like, how they reflect back in the process of reflection, how they change direction in the process of refraction, and how they interfere with other light waves. But, what do you believe happens when light waves collide with a gap? Will it go straight through the gap, or will it shift its direction? Let's investigate.
The process of bending light around corners such that it spreads out and illuminates regions where a shadow is anticipated is known as diffraction of light. In general, because both occur concurrently, it is difficult to distinguish between diffraction and interference. The diffraction of light is what causes the silver line we see in the sky. A silver line appears in the sky as the sunlight penetrates or strikes the cloud.
The double-slit experiment patterns differ from the single-slit diffraction pattern as the width and intensity reduce as we move away from the central maximum.
The path difference between two rays at an angle θ is given as ∆L= a/2 sin θ (valid only when D>> a )
The bright fringes appear at θ → sin ^-1 ( ± 3ℷ/2), sin^-1 (± 5ℷ/2)
The dark fringes appear at a sin θ = mℷ
The angular width of the central maximum is 2θ = 2λ/a
The linear width of central maxima is 2λDa.
∆L is the path difference
λ is the wavelength of the projected light
D is the distance between a slit and a screen
a is the slit width
And θ is the angle made with the undeviated direction of light.
The phenomena of light bending or diffraction may be seen in single-slit diffraction. Additionally, due to this phenomena, light from coherent sources interferes with itself, resulting in the creation of the diffraction pattern, a recognizable pattern on the screen.
For small θ, sin θ≈θ ⇒ λ = a sin θ≈aθ ⇒ θ = y/D = λ/a ⇒ y = λD/a ⇒ Width of central maximum = 2λD/a ⇒ Angular width of central maximum = 2θ = 2λ/a
###Young’s Single Slit Experiment
The double-slit experiment, carried out in 1801, proves that light is a wave. In this experiment, two tiny openings are illuminated by monochromatic light. After traveling through each slit, the waves superimpose to produce an alternative distribution of brightness and darkness on a distant screen. The brightness and size of each brilliant fringe are identical.
A similar pattern is shown on the screen when monochromatic light is fed through a single slit with a limited width in a single slit experiment. The breadth and intensity of the single-slit diffraction pattern decrease as we go away from the center maximum, in contrast to the double-slit diffraction pattern.
###Diffraction Maxima and Minima Maxima: The intersection of two wavefronts, either at their crests position or troughs position. The maximum formula is provided by dsinθ=mλ
Minima: It is the intersection of two distinct wavefronts' crests and troughs. The minima formula is provided by dsinθ= (m+1/2)λ
The distance between two succeeding bright or dark fringes is known as the fringe width. The band of alternately bright and dark material that results from interference is known as a fringe.
Q. What is the condition for constructive interference?
For the constructive interference to take place, the phase difference between the two waves must be an even multiple of pie.
Q. What is the condition for destructive interference?
For the destructive interference to take place, the phase difference between the two waves must be an odd multiple of pie.
Q. What is temporal coherence?
The average correlation between the value of a wave and itself delayed by any pair of times is known as temporal coherence.
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