A thin circular ring of mass per unit length p and radius r is rotating at an angular speed `omega` as shown in figure. The tension in the ring is

A thin circular ring of mass M and radius r is rotating about its axis with an angular speed omega . Two particles having mass m each are now attached at diametrically opposite points. The angular speed of the ring will become

A thin circular ring of mass M and radius r is rotating about its axis with an angular speed omega . Two particles having mass m each are now attached at diametrically opposite points. The angular speed of the ring will become

A thin circular ring of mass M and radius r is rotating about its axis with an angular speed omega . Two particles having mass m each are now attached at diametrically opposite points. The angular speed of the ring will become

A thin circular ring of mass M and radius r is rotating about its ais with an angular speed omega . Two particles having mas m each are now attached at diametrically opposite points. The angular speed of the ring will become

A thin circular ring of mass M and radius R is rotating about its axis with an angular speed omega_(0) two particles each of mass m are now attached at diametrically opposite points. Find new angular speed of the ring.

A ring of mass m and radius R is being rotated about its axis with angular velocity omega . If a increases then tension in ring

A thin circular right of mass M and radius R is rotating about its axis with an angular speed omega_(0) two particles each of mass m are now attached at diametrically opposite points. Find new angular speed of the ring.

A ring of radius 'r' and mass per unit length 'm' rotates with an angular velocity 'omega' in free space then tension will be :