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 \( 60^\circ \).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)