The separation between the dark lines in an interference pattern is given by the formula: \[ \Delta y = \frac{\lambda D}{d} \] Where: - \( \Delta y \) is the separation between the dark lines, - \( \lambda \) is the wavelength of the monochromatic light, - \( D \) is the distance between the slits and the screen, - \( d \) is the distance between the slits. From the formula, it is evident that the separation between the dark lines \( \Delta y \) is directly proportional to the wavelength \( \lambda \).
Thus, to increase the separation between the dark lines, we can increase the wavelength \( \lambda \).
Therefore, using monochromatic light of a longer wavelength will increase the separation between the dark lines of the interference pattern.
Figure below shows a lens of refractive index, $ \mu = 1.4 $. $ C_1 $ and $ C_2 $ are the centres of curvature of the two faces of the lens of radii of curvature 4 cm and 8 cm respectively. The lens behaves as a
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: