1) For a point on the rim of the flywheel, the distance from the center of the motion is equal to the radius of the wheel:

.
The tangential acceleration for a point on the rim is given by

where

is the angular acceleration while r is the radius. Substituting the numbers, we get

2) The radial acceleration for a point on the rim (r=0.700 m) at time t=0 is given by:

where

is the tangential velocity at time t=0.
The tangential velocity is given by

where

is the angular speed; however, at the start of the motion (t=0) the flywheel is at rest, so

and

, so the radial acceleration is

.
3) The magnitude of the acceleration at time t=0 is given by:

4) As we said at point 1), the tangential acceleration is given by

but

, the angular acceleration, is constant, so the tangential acceleration after an angle of

is just equal to the tangential acceleration at the beginning of the motion: