To solve this problem, we need to understand the diffraction pattern created by a single slit. The angle for the minima and maxima in a diffraction pattern can be determined using the formulae:
Given:
For the first minimum:
We have a \sin 30^{\circ} = 1 \times 5000 \times 10^{-10}.
Since \sin 30^{\circ} = \frac{1}{2},
a \times \frac{1}{2} = 5000 \times 10^{-10}
Thus, a = 10000 \times 10^{-10} = 10^{-6} \, \text{m}.
The first secondary maximum is approximately at the midpoint between the first and second minima:
The position of the second minimum can be calculated using a \sin \theta_2 = 2 \lambda.
10^{-6} \times \sin \theta_2 = 2 \times 5000 \times 10^{-10}
\sin \theta_2 = \frac{1}{10}
Since this is for the midpoint:
The approximate position for the secondary maximum in terms of angle is where:
\sin \theta_{\text{max}} = \frac{m + \frac{1}{2}} {a/\lambda}, with m = 1.
Calculating \theta_{\text{max}}:
\sin \theta_{\text{max}} = \frac{1.5 \lambda}{a} = \frac{1.5 \times 5000 \times 10^{-10}}{10^{-6}}
= \frac{1.5}{2} = 0.75
Thus, the angle for the first secondary maximum is \sin^{-1} (0.75) = \sin^{-1} \left( \frac{3}{4} \right).
Therefore, the correct option is \sin^{-1} \left( \frac{3}{4} \right).