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Wave Optics & Interference Formulas

Huygens principle, Young's Double Slit Experiment (YDSE), single slit diffraction, and polarization Brewster law.

8 Formulas•578+ Questions in Bank

Concept Diagram

Young's Double Slit Experiment (YDSE)
S₁S₂dScreenCentral Max (y=0)P (y)Δx = d sin θ ≈ yd/DD (Slit to Screen)Fringe Width β = λD / d | Bright: y = nλD/d | Dark: y = (2n-1)λD/(2d)
Two coherent slits S₁ and S₂ with separation d producing interference fringes on screen at distance D. Fringe width β = λD/d.

Core Formulas & Mathematical Identities

8
01

Superposition of Two Waves (Interference)

I=I1+I2+2I1I2cos⁡ϕ,Imax=(I1+I2)2,Imin=(I1−I2)2I = I_1 + I_2 + 2\sqrt{I_1 I_2}\cos\phi, \quad I_{\text{max}} = (\sqrt{I_1} + \sqrt{I_2})^2, \quad I_{\text{min}} = (\sqrt{I_1} - \sqrt{I_2})^2

Resultant intensity of two coherent wave sources with phase difference φ.

Examiner Tip: If sources are identical (I₁ = I₂ = I₀): I = 4 I₀ cos²(φ/2).
02

Young's Double Slit Experiment (YDSE)

β=λDd,yn=nλDd  (Bright),yn=(n−12)λDd  (Dark)\beta = \frac{\lambda D}{d}, \quad y_n = n \frac{\lambda D}{d} \; (\text{Bright}), \quad y_n = \left(n - \frac{1}{2}\right)\frac{\lambda D}{d} \; (\text{Dark})

Fringe width β, slit separation d, and screen distance D.

Examiner Tip: Immersing YDSE in liquid of index μ compresses fringe width to β/μ.
03

Fringe Shift by Thin Transparent Sheet

Δy=Dd(μ−1)t=(μ−1)tλβ\Delta y = \frac{D}{d}(\mu - 1)t = \frac{(\mu - 1)t}{\lambda}\beta

Lateral displacement of the whole fringe pattern when mica/glass sheet of thickness t is inserted.

Examiner Tip: Number of fringes shifted is N = (μ - 1)t / λ.
04

Single Slit Diffraction

asin⁡θ=nλ  (Minima),Central Maximum Angular Width =2λa,W=2λDaa\sin\theta = n\lambda \; (\text{Minima}), \quad \text{Central Maximum Angular Width } = \frac{2\lambda}{a}, \quad W = \frac{2\lambda D}{a}

Fraunhofer diffraction minima condition and central diffraction spread.

Examiner Tip: Width of central maximum is TWICE the width of secondary maxima.
05

Polarization (Brewster's Law & Malus' Law)

tan⁡ip=μ,I=I0cos⁡2θ\tan i_p = \mu, \quad I = I_0 \cos^2\theta

Polarizing angle where reflected and refracted rays are perpendicular, and transmitted intensity through analyzer.

Examiner Tip: When unpolarized light passes through ideal polarizer, intensity drops to I₀/2.
06

Resolving Power of Telescope & Microscope (Rayleigh)

RPtelescope=a1.22λ,RPmicroscope=2μsin⁡θ1.22λ=2 NA1.22λ\text{RP}_{\text{telescope}} = \frac{a}{1.22\lambda}, \quad \text{RP}_{\text{microscope}} = \frac{2\mu\sin\theta}{1.22\lambda} = \frac{2\,\text{NA}}{1.22\lambda}

Limit of resolution based on diffraction Airy disc overlap. a is aperture diameter; NA is numerical aperture.

Examiner Tip: Oil immersion objectives increase μ, thereby increasing resolving power of microscope.
07

Fresnel Distance (Ray vs Wave Optics Boundary)

ZF=a2λ,Ray Optics valid for D≪ZF,  Diffraction dominates for D≫ZFZ_F = \frac{a^2}{\lambda}, \quad \text{Ray Optics valid for } D \ll Z_F, \; \text{Diffraction dominates for } D \gg Z_F

Distance beyond which ray of light spreads by an amount comparable to aperture size a.

Examiner Tip: Diffraction spread is equal to aperture size a exactly when D = Z_F.
08

Thin Film Interference & Phase Shift on Reflection

2μtcos⁡r=(n+12)λ  (Reflected Maxima),2μtcos⁡r=nλ  (Reflected Minima)2\mu t \cos r = \left(n + \frac{1}{2}\right)\lambda \; (\text{Reflected Maxima}), \quad 2\mu t \cos r = n\lambda \; (\text{Reflected Minima})

Interference in reflected rays from thin dielectric film of thickness t. Extra λ/2 path shift occurs upon reflection from denser boundary (Stokes' relation).

Examiner Tip: An extremely thin soap film (t << λ) appears completely dark in reflected light.

Top Examiner Traps & Pitfalls

Frequently tested misconceptions in Wave Optics & Interference

  • •Central fringe shifts toward the side where transparent sheet is placed.
  • •In single slit diffraction, minima condition is a sin θ = nλ (looks like constructive in interference, but is DESTRUCTIVE here).