For an infinitely long wire bent into a semi-circular shape, we can use the Biot-Savart law to find the magnetic field at the center of the semi-circular loop.
The formula for the magnetic induction along the axis of a semi-circular loop of current is given by: \[ B = \frac{\mu_0 I}{4r} \] Where: - \( \mu_0 \) is the permeability of free space, - \( I \) is the current, - \( r \) is the radius of the semi-circular loop. Given that the radius is 1 m and the magnetic field along the axis is directed along the line passing through the center of the semi-circle, the magnitude of the magnetic induction is \( \frac{\mu_0 I}{4r} \).
Thus, the magnetic induction is \( \frac{\mu_0 I}{4r} \, \text{T} \).
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: