The total current is divided into two parts, one flowing through the galvanometer and the other through the shunt. The fraction of the current passing through the galvanometer is given by the ratio of the resistance of the galvanometer to the total resistance (which is the sum of the resistances of the galvanometer and the shunt): \[ I_{\text{galv}} = \frac{R_{\text{galv}}}{R_{\text{galv}} + R_{\text{shunt}}} \] Substituting the given values: \[ I_{\text{galv}} = \frac{90}{90 + 10} = \frac{90}{100} = \frac{9}{10}. \] The remaining fraction of the current flows through the shunt: \[I_{\text{shunt}} = 1 - I_{\text{galv}} = 1 - \frac{9}{10} = \frac{1}{10}. \] Thus, the fraction of the current passing through the galvanometer is \( \frac{9}{10} \) and the fraction passing through the shunt is \( \frac{1}{10} \).
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: