A bar of mass 'm' length 'l' is in pure translatory motion with its centre velocity 'v' It collides with another identical bar which is in rest and sticks to it.
Assume that after the collision it becomes one system, then the angular velocity of the system after the collision is.
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A bar of mass M and length L is in pure traslatory motion with its of mass velocity V . It collides with and sticks to a second identical bar which is initially at rest . ( Assume that it bocomes one composite bar of length 2L) . The angular velocity of the composite bar will be

A bar of mass M and length L is in pure traslatory motion with its of mass velocity V . It collides with and sticks to a second identical bar which is initially at rest . ( Assume that it bocomes one composite bar of length 2L) . The angular velocity of the composite bar will be

A bar of mass m and length l is in pure translational motion with its centre of mass moving with a velocity v. It collides and sticks to another identical bar at rest as shown in the figure. Assuming that after the collision the system of the two bars becomes one composite bar of length 2l, then the angular velocity of the composite bar will be

A bar of mass m and length l is in pure translational motion with its centre of mass moving with a velocity v. It collides and sticks to another identical bar at rest as shown in the figure. Assuming that after the collision the system of the two bars becomes one composite bar of length 2l, then the angular velocity of the composite bar will be

A body of mass 'm' moving with certain velocity collides with another identical body at rest. If the collision is perfectly elastic and after the collision both the bodies moves

A body of mass 'm' moving with certain velocity collides with another identical body at rest. If the collision is perfectly elastic and after the collision both the bodies moves