When an object traces a circular path about an axis of rotation, its motion is considered to be rotatory motion.
We categorize the problem to be rotational kinematics under constant angular acceleration.
It is given that
Angular velocity
ω=5.0rev/s=5(2πrad/s)=10πrad/s
Time of constant angular velocity t = 8 s
Time of angular retardation t’= 12 s
Equations to use
(i) angular acceleration
α=tω−ωo
(ii) angular displacement
θ=ωot+(21)αt2
Substitution of the values
When the tub is speeding up, the angular acceleration of the tub is
α1=tω−0=8s10πrad/s−0=1.25πrad/s2
The angular displacement
θ1=ωot+(21)α1t2=0+(21)(1.25πrad/s2)(8s)2=40πrad
However, one revolution
=2πrad
Therefore, the number of revolutions made by the tub in 8s when it is accelerating is
n1=2πrad/rev40πrad=20rev
When the tub is slowing down from
10πrad/s
to zero in 12 s, then the angular acceleration of the tub is
α2=t0−ω=12s0−10πrad/s=−0.833πrad/s2
The angular displacement
θ2=ωot+(21)α2t2=(10rad/s)(12s)+(21)(−0.833πrad/s2)(12s)2=120πrad−60πrad=60πrad
Therefore, the number of revolutions made by the tub in 12s when it is decelerating is
n2=2πrad/rev60πrad=30rev
The total number of revolutions the tub makes when it is in motion
= 20 rev + 30 rev
= 50 rev
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