The angular position of the first dark fringe in a single-slit diffraction pattern is given by: \[ \sin \theta = \frac{m\lambda}{a} \] Where:
- \( \lambda \) is the wavelength of the light,
- \( a \) is the width of the slit,
- \( m \) is the order of the dark fringe (for the first dark fringe, \( m = 1 \)).
Given: - \( \lambda = 800 \, \text{nm} = 800 \times 10^{-9} \, \text{m} \),
- \( a = 0.5 \, \text{mm} = 0.5 \times 10^{-3} \, \text{m} \),
- The distance to the screen is \( L = 1.5 \, \text{m} \).
The angle for the first dark fringe can be calculated by: \[ \sin \theta = \frac{800 \times 10^{-9}}{0.5 \times 10^{-3}} = 1.6 \times 10^{-3} \] Now, the linear distance between the first dark fringes is given by: \[ y = 2L \tan \theta \approx 2L \sin \theta \quad \text{(for small angles, } \tan \theta \approx \sin \theta) \] Substituting the values: \[ y = 2 \times 1.5 \times 1.6 \times 10^{-3} = 4.8 \times 10^{-3} \, \text{m} = 4.8 \, \text{mm} \]
Thus, the distance between the first dark fringes on either side of the central bright fringe is \( 4.8 \, \text{mm} \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: