Wave Optics: Numerical Problems Set (5)

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Question

In Young’s double-slit experiment, the slits are d=0.5 mmd = 0.5 \text{ mm} apart and the screen is D=1.5 mD = 1.5 \text{ m} away. Light of wavelength λ=600 nm\lambda = 600 \text{ nm} is used. Find (a) the fringe width, (b) the position of the 5th bright fringe from the center, (c) the new fringe width if the entire setup is dipped in water (refractive index n=4/3n = 4/3).

Solution — Step by Step

β=λDd\beta = \frac{\lambda D}{d}

Plug in: β=600×109×1.50.5×103=9×1070.5×103=1.8×103 m=1.8 mm\beta = \frac{600 \times 10^{-9} \times 1.5}{0.5 \times 10^{-3}} = \frac{9 \times 10^{-7}}{0.5 \times 10^{-3}} = 1.8 \times 10^{-3} \text{ m} = 1.8 \text{ mm}.

yn=nβy_n = n\beta. For n=5n = 5: y5=5×1.8=9 mmy_5 = 5 \times 1.8 = 9 \text{ mm} from the central maximum.

Inside water, wavelength becomes λ=λ/n=600/(4/3)=450 nm\lambda' = \lambda/n = 600/(4/3) = 450 \text{ nm}.

Geometry (dd and DD) doesn’t change. Fringe width scales with λ\lambda:

β=λD/d=(3/4)β=0.75×1.8=1.35 mm\beta' = \lambda' D / d = (3/4) \beta = 0.75 \times 1.8 = 1.35 \text{ mm}.

Final answers: β=1.8 mm\beta = \mathbf{1.8 \text{ mm}}, y5=9 mmy_5 = \mathbf{9 \text{ mm}}, β=1.35 mm\beta' = \mathbf{1.35 \text{ mm}}.

Why This Works

Fringe width depends on the wavelength inside the medium where interference happens. Light slows down in water (frequency unchanged, vv drops, so λ\lambda drops by factor nn). Closer-spaced wavelengths mean closer-spaced fringes.

Path difference at the screen depends on dsinθdy/Dd \sin\theta \approx dy/D — pure geometry, so dd and DD don’t change with the medium. Only λ\lambda changes.

Alternative Method

For part (c), since β=β/n\beta' = \beta/n, we can write the answer immediately as 1.8/(4/3)=1.35 mm1.8/(4/3) = 1.35 \text{ mm}. No need to recompute λ\lambda' separately.

Common Mistake

Many students think dipping the setup in water changes DD or dd via “optical path length” tricks. It doesn’t — the slits and screen are physical objects at fixed positions. Only the wavelength of the light traveling between them changes (becomes λ/n\lambda/n). That’s what shrinks the fringes.

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