Question:

In a single slit diffraction experiment, the aperture of the slit is 3 mm and the separation between the slit and the screen is 1.5 m. A monochromatic light of wavelength 600 nm is normally incident on the slit. Calculate the distance of (I) first order minimum, and (II) second order maximum, from the centre of the screen.

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In single-slit diffraction, minima occur at \( a \sin \theta = m\lambda \), and secondary maxima lie roughly midway between them. Use small angle approximation \( \sin \theta \approx \frac{y}{D} \) for small diffraction angles.
Updated On: Jun 17, 2025
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Solution and Explanation

Given: - Slit width \( a = 3\,\text{mm} = 3 \times 10^{-3}\,\text{m} \) - Distance to screen \( D = 1.5\,\text{m} \) - Wavelength \( \lambda = 600\,\text{nm} = 600 \times 10^{-9}\,\text{m} \) \underline{(I) First Order Minimum:}
For single slit diffraction, the minima occur at: \[ a \sin \theta = m\lambda \quad \text{for } m = \pm 1, \pm 2, \ldots \] For small angles, \( \sin \theta \approx \tan \theta = \frac{y}{D} \), \[ a \cdot \frac{y_1}{D} = \lambda \Rightarrow y_1 = \frac{\lambda D}{a} = \frac{600 \times 10^{-9} \times 1.5}{3 \times 10^{-3}} = 3 \times 10^{-4}\,\text{m} = 0.3\,\text{mm} \] Distance of first order minimum = \( \boxed{0.3\,\text{mm}} \) \underline{(II) Second Order Maximum (Approximate):}
Secondary maxima in single slit are not sharp and lie approximately midway between two minima. So, second order maximum lies roughly between 1st and 2nd minima: \[ \text{Position of 2nd minimum: } y_2 = \frac{2\lambda D}{a} = \frac{2 \times 600 \times 10^{-9} \times 1.5}{3 \times 10^{-3}} = 0.6\,\text{mm} \] \[ \text{Approximate position of 2nd maximum: } y \approx \frac{y_1 + y_2}{2} = \frac{0.3 + 0.6}{2} = 0.45\,\text{mm} \] Distance of second order maximum \( \approx \boxed{0.45\,\text{mm}} \)
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