Step 1: The condition for the first minimum in the diffraction pattern produced by a single slit is: \[ d \sin \theta = m \lambda \quad {where} \quad m = 1 \, ({first minimum}) \] Step 2: Substitute the given values:
- \( \lambda = 4500 \, {Å} = 4500 \times 10^{-10} \, {m} \),
- \( \theta = 30^\circ \). \[ d \sin 30^\circ = 4500 \times 10^{-10} \]
Step 3: Since \( \sin 30^\circ = 0.5 \), the equation becomes: \[ d \times 0.5 = 4500 \times 10^{-10} \] Step 4: Solving for \( d \): \[ d = \frac{4500 \times 10^{-10}}{0.5} = 9 \times 10^{-6} \, {m} = 0.9 \, \mu {m} \] Thus, the width of the slit is \( 0.9 \, \mu {m} \).
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by