haya.Learning made clear
Unit X · Wave optics
7 min readConcept sheet1-mark MCQ and assertion-reason, 2-mark 'how does the central maximum change if...', and short numericals; also a NEET favourite

Width of the central maximum (qualitative)

The central maximum stretches between the first minima on either side. It widens when the slit is narrower or the wavelength is longer.

Angular width of central maximum2λ/a (from −λ/a to +λ/a)
Linear width on a screen at distance D2λD/a
Width of a secondary maximumAbout half the central maximum, λD/a
DependenceWidth ∝ λ and ∝ D, but ∝ 1/a

Where the central maximum ends

The central maximum lies between the first minimum on each side, at θ = +λ/a and θ = −λ/a. So its angular width is 2λ/a. On a screen at distance D, its linear width is 2λD/a. We use these results without derivation. Each secondary maximum is only about half as wide. The key idea is simple: the narrower the slit, the more the light spreads.

How the central maximum changes

ChangeEffect on the central maximumReason
Slit made narrower (smaller a)Wider and fainterWidth 2λD/a ∝ 1/a, and less light passes
Slit made much wider than λVery narrow; light goes almost straightSpreading becomes negligible, so ray optics holds
Red light in place of blue lightWiderRed light has the longer wavelength
Screen moved farther away (larger D)Wider on the screen; angular width unchangedLinear width 2λD/a ∝ D
Whole set-up dipped in waterNarrowerThe wavelength in water is λ/μ
White light usedWhite centre with coloured edgesEach colour has its own width; red spreads the most

Interference vs diffraction

Interference (double slit)Superposition of waves from two coherent sources. Fringes are equally wide (β = λD/d). Bright fringes are about equally bright.
Diffraction (single slit)Superposition of wavelets from different parts of one wavefront. The central maximum is twice as wide as the others (2λD/a). Brightness falls off quickly away from the centre.

In Young's experiment each slit also diffracts, so the interference fringes are seen inside the broad single slit pattern.

Worked example: width of the central maximum

Problem

Light of wavelength 600 nm falls on a slit of width 0.2 mm. The screen is 1 m away. Find (a) the angular width and (b) the linear width of the central maximum. (c) What is the linear width if the slit width is doubled?

Working
  1. Given: λ = 6 × 10⁻⁷ m, a = 2 × 10⁻⁴ m, D = 1 m.
  2. (a) Angular width = 2λ/a = 2 × (6 × 10⁻⁷ m) ÷ (2 × 10⁻⁴ m) = 6 × 10⁻³ rad.
  3. (b) Linear width = 2λD/a = 6 × 10⁻³ × 1 m = 6 × 10⁻³ m = 6 mm.
  4. (c) Width ∝ 1/a, so doubling a halves the width: 6 mm ÷ 2 = 3 mm.
Answer

(a) 6 × 10⁻³ rad; (b) 6 mm; (c) 3 mm

In real life

In a pinhole camera made from a shoebox in school, making the hole too small blurs the image, because light spreads out by diffraction. The same spreading limits how much detail cameras and telescopes can show, which is why their lenses are made wide.

Exam angle

2 marks: “How does the width of the central maximum change when (a) the slit width is halved, (b) blue light is replaced by red light?” (a) It doubles, because width ∝ 1/a. (b) It increases, because width ∝ λ and red light has a longer wavelength.

2 marks: “Give two differences between the interference pattern of Young's experiment and the diffraction pattern of a single slit.” Interference: equal fringe widths, bright fringes about equally bright, two coherent sources. Diffraction: central maximum twice as wide, brightness falls quickly, wavelets from one wavefront.

3 marks: “Light of wavelength 500 nm falls on a slit of width 0.25 mm, and the screen is 1.5 m away. Find the width of the central maximum.” Width = 2λD/a = 2 × (5 × 10⁻⁷) × 1.5 ÷ (2.5 × 10⁻⁴) m = 6 × 10⁻³ m = 6 mm.

Remember it

Narrow slit, wide centre. Width = 2λD/a, with the slit width a downstairs.