To determine the angular spread of the central maxima in a single-slit diffraction pattern, we use the formula for the angular width of the central maximum:
\(\theta = 2 \times \sin^{-1} \left( \frac{\lambda}{a} \right)\)
where:
Given:
Substitute these values into the formula:
\(\theta = 2 \times \sin^{-1} \left( \frac{0.02}{0.04} \right)\)
\(\theta = 2 \times \sin^{-1} (0.5)\)
Since \(\sin^{-1} (0.5) = 30\degree\),
\(\theta = 2 \times 30\degree = 60\degree\)
Thus, the angular spread of the central maxima is \(60\degree\).
Therefore, the correct answer is \(60\degree\).
Given: - Wavelength of the microwave: \( \lambda = 2.0 \, \text{cm} = 0.02 \, \text{m} \) - Width of the slit: \( a = 4.0 \, \text{cm} = 0.04 \, \text{m} \) - Distance from the slit to the screen is irrelevant for angular spread calculation.
The angular position \( \theta \) of the first minimum in a single-slit diffraction pattern is given by: \[ a \sin \theta = m \lambda \] where: - \( m = 1 \) for the first minimum. Substituting the given values: \[ 0.04 \sin \theta = 1 \times 0.02 \] \[ \sin \theta = \frac{0.02}{0.04} \] \[ \sin \theta = 0.5 \] Thus: \[ \theta = \sin^{-1}(0.5) = 30^\circ \]
The angular spread of the central maximum is given by \( 2\theta \): \[ \text{Angular spread} = 2 \times 30^\circ = 60^\circ \]
The angular spread of the central maxima of the diffraction pattern is \( 60^\circ \).

