Related Formula
a θₙ = n λ$$a \sin\theta_n = n \lambda$$
θₐₚₚᵣₒₓ = n (λ)/(a) (for small angles)$$\theta_{\text{approx}} = n \frac{\lambda}{a} \quad \text{(for small angles)}$$
Core Logic
Let the width of the slit be a$a$, and the light wavelength be λ = 628~nm = 628 × 10⁻⁹~m$\lambda = 628\mathrm{~nm} = 628 \times 10^{-9}\mathrm{~m}$.
The second minimum (n = 2$n = 2$) is located at angular position:
θ₁ = (2λ)/(a)$$\sin\theta_1 = \frac{2\lambda}{a}$$
The third minimum (n = 3$n = 3$) is located at angular position:
θ₂ = (3λ)/(a)$$\sin\theta_2 = \frac{3\lambda}{a}$$
The total angular separation is 30°$30^{\circ}$:
θ₁ + θ₂ = 30° = (π)/(6)~rad$$\theta_1 + \theta_2 = 30^{\circ} = \frac{\pi}{6}\mathrm{~rad}$$
Using the small-angle approximation (where θ ≈ θ$\theta \approx \sin\theta$):
θ₁ + θ₂ ≈ (2λ)/(a) + (3λ)/(a) = (5λ)/(a)$$\theta_1 + \theta_2 \approx \frac{2\lambda}{a} + \frac{3\lambda}{a} = \frac{5\lambda}{a}$$
Equating to the given separation:
(5λ)/(a) = (π)/(6) a = (30λ)/(π)$$\frac{5\lambda}{a} = \frac{\pi}{6} \implies a = \frac{30\lambda}{\pi}$$
Substitute the given values (using π ≈ 3.14$\pi \approx 3.14$):
a = 30 × 628 × 10⁻⁹~m3.14 = 30 × 200 × 10⁻⁹~m = 6 × 10⁻⁶~m = 6~μ m$$a = \frac{30 \times 628 \times 10^{-9}\mathrm{~m}}{3.14} = 30 \times 200 \times 10^{-9}\mathrm{~m} = 6 \times 10^{-6}\mathrm{~m} = 6\mathrm{~\mu m}$$
Step 1: Final Conclusion
The width of the slit is 6~μ m$6\mathrm{~\mu m}$.
Pattern Recognition
In single slit diffraction, the position of minima is a θ = n λ$a \sin\theta = n \lambda$. The angular spread from the n₁$n_1$-th minimum on one side to the n₂$n_2$-th minimum on the other is (n₁ + n₂) (λ)/(a)$(n_1 + n_2) \frac{\lambda}{a}$. Since π ≈ 3.14$\pi \approx 3.14$, note how 628 / 3.14 = 200$628 / 3.14 = 200$, resolving to a neat integer.
Chapter Mix
Class 12 Physics: Wave Optics