We need to find the tension in the longer string. We know that the stone is hanging at equilibrium, so the forces in the vertical and horizontal directions must balance.
Let the tensions in the two strings be \( T_1 \) (the shorter string) and \( T_2 \) (the longer string).
The forces in the vertical direction are: \[ T_1 \sin(60^\circ) + T_2 \sin(30^\circ) = mg \] Substituting the known values: \[ T_1 \sin(60^\circ) + T_2 \sin(30^\circ) = 2 \times 10 \] \[ T_1 \cdot \frac{\sqrt{3}}{2} + T_2 \cdot \frac{1}{2} = 20 \] The forces in the horizontal direction must balance: \[ T_1 \cos(60^\circ) = T_2 \cos(30^\circ) \] \[ T_1 \cdot \frac{1}{2} = T_2 \cdot \frac{\sqrt{3}}{2} \] \[ T_1 = \sqrt{3} T_2 \] Substitute \( T_1 = \sqrt{3} T_2 \) into the vertical force equation: \[ \sqrt{3} T_2 \cdot \frac{\sqrt{3}}{2} + T_2 \cdot \frac{1}{2} = 20 \] \[ \frac{3}{2} T_2 + \frac{1}{2} T_2 = 20 \] \[ 2 T_2 = 20 \] \[ T_2 = 10 \, \text{N} \] Thus, the tension in the longer string is \( T_2 = 10 \, \text{N} \).
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: