Saif Ullah B. answered 02/11/20
Physics and Mathematics Tutor
(a) Start of the motion or t = 0,
At this instance, the flywheel is at rest. All velocities, linear or angular are zero everywhere. The angular acceleration α is non-zero. So we get
radial acceleration of a point on the rim = - ω2 r (positive direction is radially outward from the center) = 0 (rest)
tangential acceleration of a point on the rim = α x r (perpendicular to the radius vector at the point on the rim).
By the way, the angular acceleration α and radius vector to any point on the rim r are always perpendicular in this problem. So the tangential acceleration is always perpendicular to r
resultant acceleration = sum of previous 2 quantities = α x r = 90 degrees to the radius vector r.
(b) flywheel rotates through 120 degrees or 2π/3 radians. The time T it takes to do that is related to the magnitude of α through:
θ = α T2 / 2.
From T, the magnitude of the angular velocity at time T can be computed via:
ω = α T.
The various accelerations can now be computed as follows
radial = - ω2 r (non-zero unlike in part (a), directed inward toward the center)
tangential = α x r (magnitude is just the product of values of α and r, direction is perpendicular to r in the direction wheel is turning, same as part (a))
resultant = -ω2 r + α x r
The resultant acceleration in part (b) is better computed by drawing the vector diagram. The radial and tangential accelerations are legs of a right triangle. The magnitude is length of hypotenuse. The direction can be computed using an appropriate trig ratio e.g.
tan γ = (magnitude of tangential) / (magnitude of radial)
where γ is the angle of the resultant with the radial.