A wheel is rolling without slipping on a horizontal plane with velocity `v` and acceleration `a` of centre of mass as shown in figure. Acceleration at

The acceleration of centre of mass of system as shown in figure is

A wheel is rolling on a horizontal plane. At a certain instant it has a velocity v and acceleration a of CM as shown in figure . Acceleration of

A wheel is rolling on a horizontal plane. At a certain instant it has a velocity v and acceleration a of CM as shown in figure . Acceleration of

A disc having radius R is rolling without slipping on a horizontal ( x-z ) plane. Centre of the disc has a velocity v and acceleration a as shown. Speed of point P having coordinates (x,y) is

A disc having radius R is rolling without slipping on a horizontal ( x-z ) plane. Centre of the disc has a velocity v and acceleration a as shown. Speed of point P having coordinates (x,y) is

A disc having radius R is rolling without slipping on a horizontal ( x-z ) plane. Centre of the disc has a velocity v and acceleration a as shown. If v=sqrt(2aR) the angle theta between acceleration of the top most point and the horizontal is

A disc having radius R is rolling without slipping on a horizontal ( x-z ) plane. Centre of the disc has a velocity v and acceleration a as shown. If v=sqrt(2aR) the angle rho between acceleration of the top most point and the horizontal is

A ring of radius R rolls on a horizontal surface with constant acceleration a of the centre of mass as shown in figure. If omega is the instantaneous angular velocity of the ring. Then the net acceleration of the point of contact of the ring with gound is

A ring of radius R rolls on a horizontal surface with constant acceleration a of the centre of mass as shown in figure. If omega is the instantaneous angular velocity of the ring. Then the net acceleration of the point of contact of the ring with gound is