1. Chapter at a Glance
Wave optics explains effects that ray optics cannot: interference, diffraction and polarisation. They show that light is a wave. The chapter covers Huygens' principle, coherent sources, Young's double-slit experiment (YDSE), single-slit diffraction, resolving power and polarisation (Malus's and Brewster's laws). JEE Main asks one question almost every year, usually on YDSE fringe width or intensity.
- Fringe width and fringe positions in YDSE; effect of a medium or a thin sheet.
- Resultant intensity and Imax/Imin for unequal sources.
- Width of the central maximum in single-slit diffraction.
- Malus's law and Brewster's angle.
2. Huygens' Principle
- Every point on a wavefront acts as a source of secondary wavelets; the new wavefront is the forward envelope of these wavelets.
- It explains the laws of reflection and refraction, and predicts that light slows down in a denser medium (v = c/n) — confirmed by experiment.
- Point source → spherical wavefronts; distant source → plane wavefronts.
3. Interference and YDSE
- Coherent sources have a constant phase difference (same frequency). Two independent bulbs are not coherent. YDSE gets coherence by dividing one wavefront.
- Resultant intensity: I = I₁ + I₂ + 2√(I₁I₂) cosφ. For equal intensities, I = 4I₀ cos²(φ/2).
- Imax/Imin = [(√I₁ + √I₂)/(√I₁ − √I₂)]² = [(a₁ + a₂)/(a₁ − a₂)]².
- Path difference Δ = yd/D. Bright fringe: Δ = nλ; dark fringe: Δ = (2n − 1)λ/2.
- Fringe width β = λD/d; in a medium of index μ, β′ = β/μ.
- A thin sheet (thickness t, index μ) in front of one slit shifts the whole pattern by (μ − 1)tD/d towards that slit; number of fringes shifted = (μ − 1)t/λ.
- With white light, the central fringe is white and the others are coloured.
4. Diffraction and Resolving Power
- Diffraction is the bending of light around an obstacle or slit comparable in size to λ.
- Single slit of width a: minima at a sinθ = nλ (n = 1, 2, …). The central maximum has angular width 2λ/a and linear width 2λD/a — twice the width of the secondary maxima.
- Narrowing the slit widens the central maximum.
- Resolving power: the smallest angle a telescope can resolve is θ ≈ 1.22λ/D (D = aperture diameter). Larger apertures and shorter wavelengths resolve finer detail. A microscope's resolving power is 2n sinθ/1.22λ.
5. Polarisation
- Polarisation proves that light is a transverse wave (sound cannot be polarised).
- Unpolarised light through a polariser: intensity halves.
- Malus's law: I = I₀cos²θ for polarised light through an analyser at angle θ.
- Brewster's law: at the polarising angle, tan θp = n; the reflected light is completely polarised and the reflected and refracted rays are perpendicular (θp + r = 90°).
- Uses: Polaroid sunglasses reduce glare; 3D movies; stress analysis.
6. Formula Master Table
| Quantity | Formula |
|---|---|
| Resultant intensity | I = I₁ + I₂ + 2√(I₁I₂) cosφ |
| Intensity ratio | Imax/Imin = ((a₁ + a₂)/(a₁ − a₂))² |
| Fringe width | β = λD/d |
| nth bright / dark | y = nβ; y = (2n − 1)β/2 |
| Sheet shift | (μ − 1)tD/d |
| Single slit central max | 2λD/a |
| Resolution limit | θ = 1.22λ/D |
| Malus / Brewster | I = I₀cos²θ; tanθp = n |
7. Mind Map
- Wavefronts
- Reflection, refraction
- Coherence
- YDSE, β = λD/d
- Thin sheet shift
- Single slit
- Resolving power
- Malus's law
- Brewster's angle
8. Tips and Tricks
- Intensity ratio 9 : 1 means amplitude ratio 3 : 1, so Imax/Imin = (4/2)² = 4.
- When two wavelengths are used, bright fringes coincide where n₁λ₁ = n₂λ₂ — use the LCM.
- Immersing YDSE in water shrinks β by the factor μ.
- Two crossed polarisers block light; a third one at 45° between them lets I₀/8 through.
- Forgetting to halve unpolarised light at the first polariser.
- Using D for slit separation (d) or vice versa.
- Thinking the central maximum in single-slit diffraction has the same width as the others.
9. Important One-liners
- Interference needs coherent sources.
- Energy is conserved in interference; it is only redistributed.
- Polarisation shows that light waves are transverse.
- At Brewster's angle the reflected and refracted rays are perpendicular.
- Diffraction is noticeable when the obstacle size is comparable to the wavelength.
- A bigger telescope aperture gives better resolution.
10. Solved Numericals: Average to Advanced
Five average-level and five advanced-level problems. Click to reveal each answer and its full working.
Average level
In YDSE, λ = 600 nm, slit separation d = 1 mm and screen distance D = 1 m. Find the fringe width.
Show answer & solution
Concept: β = λD/d.
- β = 600 × 10⁻⁹ × 1/10⁻³.
- = 6 × 10⁻⁴ m = 0.6 mm.
Answer: 0.6 mm
The apparatus of N1 is immersed in water (μ = 4/3). Find the new fringe width.
Show answer & solution
Concept: λ in water = λ/μ, so β′ = β/μ.
- β′ = 0.6/(4/3) = 0.6 × 0.75.
- = 0.45 mm.
Answer: 0.45 mm
Light of wavelength 500 nm passes through a single slit 0.1 mm wide onto a screen 2 m away. Find the width of the central maximum.
Show answer & solution
Concept: width = 2λD/a.
- Width = 2 × 5 × 10⁻⁷ × 2/10⁻⁴.
- = 0.02 m = 2 cm.
Answer: 2 cm
Find Brewster's angle for glass of refractive index √3, and the angle of refraction at that incidence.
Show answer & solution
Concept: tanθp = n; θp + r = 90°.
- tanθp = √3 ⇒ θp = 60°.
- r = 90° − 60° = 30°.
Answer: 60°; 30°
Unpolarised light of intensity I₀ passes through two polarisers whose axes are at 60°. Find the transmitted intensity.
Show answer & solution
Concept: first polariser halves; then Malus's law.
- After the first: I₀/2.
- After the second: (I₀/2)cos²60° = (I₀/2)(1/4).
- = I₀/8.
Answer: I₀/8
Advanced level
Two coherent sources have intensities in the ratio 9 : 1. Find the ratio of maximum to minimum intensity in their interference pattern.
Show answer & solution
Concept: amplitude ∝ √intensity.
- a₁ : a₂ = 3 : 1.
- Imax ∝ (3 + 1)² = 16; Imin ∝ (3 − 1)² = 4.
- Ratio = 4 : 1.
Answer: 4 : 1
In YDSE with λ = 600 nm, a thin glass sheet (μ = 1.5) placed over one slit shifts the central fringe by 5 fringes. Find the sheet's thickness.
Show answer & solution
Concept: extra path (μ − 1)t = number of fringes × λ.
- (1.5 − 1)t = 5 × 600 × 10⁻⁹.
- t = 3 × 10⁻⁶/0.5 = 6 × 10⁻⁶ m.
- = 6 μm.
Answer: 6 μm
For the set-up of N1 (β = 0.6 mm), find the distance from the centre of (a) the 3rd bright fringe, (b) the 3rd dark fringe, and (c) the separation between them.
Show answer & solution
Concept: bright y = nβ; dark y = (2n − 1)β/2.
- (a) y₃(bright) = 3 × 0.6 = 1.8 mm.
- (b) y₃(dark) = 5 × 0.6/2 = 1.5 mm.
- (c) Separation = 0.3 mm (= β/2).
Answer: 1.8 mm; 1.5 mm; 0.3 mm
A YDSE (d = 1 mm, D = 1 m) is lit by 600 nm and 400 nm together. Find the nearest point to the centre where bright fringes of both wavelengths coincide.
Show answer & solution
Concept: coincidence when n₁λ₁ = n₂λ₂.
- 600n₁ = 400n₂ ⇒ n₁/n₂ = 2/3; smallest: n₁ = 2, n₂ = 3.
- y = n₁λ₁D/d = 2 × 600 × 10⁻⁹ × 1/10⁻³.
- y = 1.2 × 10⁻³ m = 1.2 mm.
Answer: 1.2 mm from the centre
A telescope has an objective of diameter 10 cm. Find the smallest angular separation it can resolve for light of 500 nm. Would doubling the diameter help?
Show answer & solution
Concept: Rayleigh criterion θ = 1.22λ/D.
- θ = 1.22 × 5 × 10⁻⁷/0.1.
- = 6.1 × 10⁻⁶ rad (about 1.3 arc-seconds).
- Doubling D halves θ — the telescope resolves twice as finely.
Answer: about 6.1 × 10⁻⁶ rad; yes, it halves the limit
11. PYQ-pattern Questions with Solutions
These questions are original and modelled on concepts frequently tested in JEE Main.
Two sources are coherent if they have:
- Same amplitude only
- Constant phase difference
- Different frequencies
- Same intensity only
Show solution
Coherence requires the same frequency and a constant phase difference.
Answer: (B)
Which phenomenon proves that light is a transverse wave?
- Interference
- Diffraction
- Polarisation
- Reflection
Show solution
Only transverse waves can be polarised.
Answer: (C)
In YDSE, the slit separation is doubled and the screen distance is halved. The fringe width becomes:
- Unchanged
- Half
- One-fourth
- Four times
Show solution
β ∝ D/d = (1/2)/2 = 1/4.
Answer: (C)
In interference, the energy at dark fringes:
- Is destroyed
- Is converted to heat
- Is redistributed to bright fringes
- Goes back to the source
Show solution
Energy is conserved; average intensity over the pattern equals I₁ + I₂. Bright fringes get the missing energy.
Answer: (C)
Find Brewster's angle (in degrees) for a medium of refractive index √3.
Show solution
tanθp = √3 ⇒ 60°.
Answer: 60
Two coherent waves each of intensity I₀ interfere with phase difference 60°. Find the resultant intensity in units of I₀.
Show solution
I = 4I₀cos²(30°) = 4I₀ × 3/4 = 3I₀.
Answer: 3
12. Quick Revision Summary
- Huygens: secondary wavelets; v = c/n in a medium.
- I = I₁ + I₂ + 2√(I₁I₂)cosφ; Imax/Imin = ((a₁ + a₂)/(a₁ − a₂))².
- β = λD/d; β/μ in a medium; sheet shift (μ − 1)tD/d.
- Single slit: central width 2λD/a; resolution 1.22λ/D.
- Malus I₀cos²θ; Brewster tanθp = n.