The net acceleration \( a_{\text{net}} \) can be expressed as the vector sum of the tangential acceleration \( a_t \) and the centripetal acceleration \( a_c \). The centripetal acceleration is given by: \[ a_c = \frac{v^2}{r} \] Where:
- \( v \) is the instantaneous speed of the ball,
- \( r = 5 \, \text{m} \) is the radius. Given:
- The tangential acceleration \( a_t = 10 \, \text{m/s}^2 \),
- The angle between the net acceleration and the centripetal acceleration is \( 30^\circ \). Using the relation for the net acceleration: \[ a_{\text{net}}^2 = a_c^2 + a_t^2 \] Also, the net acceleration is related to the angle \( \theta \) between the tangential and centripetal accelerations: \[ a_{\text{net}} = \sqrt{a_t^2 + a_c^2} \] Since \( \theta = 30^\circ \), the tangent of the angle gives: \[ \tan(30^\circ) = \frac{a_t}{a_c} \] This gives: \[ \frac{10}{a_c} = \tan(30^\circ) = \frac{1}{\sqrt{3}} \] Solving for \( a_c \): \[ a_c = 10\sqrt{3} \, \text{m/s}^2 \] Now substitute the value of \( a_c \) into the centripetal acceleration formula: \[ a_c = \frac{v^2}{r} \Rightarrow 10\sqrt{3} = \frac{v^2}{5} \] Solving for \( v \): \[ v^2 = 50\sqrt{3} \] \[ v = \sqrt{50\sqrt{3}} \approx 9.3 \, \text{m/s} \]
Thus, the instantaneous speed is \( 9.3 \, \text{m/s} \).
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: