Wave Optics — NEET Physics Notes
Wave optics covers the wave nature of light — interference, diffraction, polarisation, and Young’s double slit experiment. This chapter connects to modern physics and frequently appears in NEET with significant weightage.
Quick Revision
- Huygens’ Principle: Every point on a wavefront is a source of secondary wavelets
- Interference: Superposition of two coherent light waves — constructive and destructive
- Young’s Double Slit: Fringe width β = λD/d; bright fringes: d sinθ = mλ
- Diffraction: Bending of light around obstacles — single slit: a sinθ = mλ
- Polarisation: Restriction of vibration to one plane — proves light is transverse
- Brewster’s Law: tan θ_B = n₂/n₁; at polarising angle, reflected and refracted rays are perpendicular
- Malus Law: I = I₀ cos²θ (intensity through analyser)
Standard Study
Nature of Light
- Light is a transverse electromagnetic wave
- Newton’s corpuscular theory was disproved by wave theory (interference, diffraction)
- Huygens’ wave theory explained reflection, refraction, interference
- Maxwell proved light is electromagnetic wave — speed = 3 × 10⁸ m/s in vacuum
Huygens’ Principle
- Secondary wavelets from each point on wavefront travel at speed c
- New wavefront is tangent to all secondary wavelets
- Explains laws of reflection and refraction
- Cannot explain polarisation (light is transverse)
Interference
Coherent Sources: Sources with same frequency and constant phase difference
Young’s Double Slit Experiment:
- Fringe width: β = λD/d
- Distance between centres of consecutive bright fringes
- Dark fringe position: d sinθ = (m + ½)λ
- Bright fringe position: d sinθ = mλ
Result: Alternating bright and dark fringes on screen
Angular Fringe Width: θ = λ/d (for small angles)
Conditions for Interference:
- Sources must be coherent
- Sources must have same frequency
- Phase difference must remain constant
Diffraction
Single Slit Diffraction:
- Central maximum is brightest and widest
- Minima: a sinθ = mλ (m = ±1, ±2, …)
- Width of central maximum: 2λD/a
- Resolving power of optical instruments depends on diffraction
Difference between Interference and Diffraction:
- Interference: two or more waves superimpose
- Diffraction: single wave bends around obstacle/slit
Polarisation
- Proof that light is a transverse wave
- Natural light is unpolarised — vibrations in all directions
- Polarised light: vibrations in one direction only
Methods of Polarisation:
- Polaroid sheets (selective absorption)
- Reflection at Brewster’s angle (tan θ_B = n)
- Refraction through doubly refracting crystal (Calcite, Quartz)
- Scattering
Brewster’s Law:
- At Brewster’s angle θ_B: reflected ray is completely polarised
- tan θ_B = n₂/n₁
- At this angle: reflected and refracted rays are perpendicular
Malus Law:
- I = I₀ cos²θ
- Maximum intensity when polariser and analyser are parallel
- Zero intensity when they are perpendicular
Applications of Polarisation
- Polaroid sunglasses (reduce glare)
- LCD displays
- Optical activity (sugar solution, rotation of plane of polarisation)
- Stress analysis in transparent materials
Deep Study
Resolving Power
- Rayliegh criterion: Two points are just resolved when central maximum of one falls on first minimum of the other
- Resolving power of microscope = 1/(1.22 λ)
- Telescope resolving power improves with larger aperture
Double Refraction
- Uniaxial crystals: one optic axis (Calcite, Tourmaline)
- Double refraction: ordinary and extraordinary rays
- Nicol prism: used as polariser and analyser
- Huygens’ construction for double refraction
Optical Activity
- Plane of polarisation rotates when passed through certain substances
- Specific rotation: α = [θ]/(l × c)
- Dextrorotatory: rotates plane to the right (+)
- Laevorotatory: rotates plane to the left (−)
- Sucrose solution is laevorotatory
Interference in Thin Films
- Reflected light from top and bottom surfaces of thin film interferes
- Constructive: 2μt cos r = (m + ½)λ (bright)
- Destructive: 2μt cos r = mλ (dark)
- Produces colours in soap bubbles, oil films
Lloyd’s Mirror
- Interference between direct ray and reflected ray from a mirror
- Fringe pattern similar to double slit
- Path difference = r − l + λ/2 (phase reversal on reflection from denser medium)
Exam Tips
- Young’s double slit: β = λD/d — increasing D or decreasing d increases fringe width
- Diffraction through single slit: central maximum is twice as wide as other maxima
- Polarisation proves light is transverse — longitudinal waves cannot be polarised
- Brewster’s angle: tan θ_B = n — reflected light is completely polarised
- Malus Law: I = I₀ cos²θ — intensity varies with square of cosine
- Interference: always two or more coherent sources; diffraction: single source
- Thin film interference: account for phase change of π on reflection from denser medium
- Optical rotation: polarisation plane rotation by sugar solution — dextrorotatory vs laevorotatory
Common Pitfalls
- Confusing fringe width β with angular fringe width
- Forgetting phase change of π on reflection (like from denser medium)
- Confusing interference and diffraction patterns
- Not knowing when reflected light from thin film is totally destructive
- Mixing up Brewster’s angle formula with Snell’s law
- Forgetting that polarisation is only for transverse waves
Suggested Study Order
- Nature of light — Huygens’ principle
- Interference — Young’s double slit experiment
- Fringe width and position formulas
- Diffraction — single slit pattern
- Polarisation and Malus law
- Brewster’s law and applications
- Thin film interference
- Resolving power and optical activity