A body rotating with constant angular velocity ω_0 = 4 rad/s…
A body rotating with constant angular velocity $\omega_0 = 4\ \mathrm{rad/s}$ begins to decelerate at $\alpha = 0.5\ \mathrm{rad/s^2}$. Find its angular velocity (a) after $t = 1\ \mathrm{s}$; (b) after turning through $\theta = \pi/3\ \mathrm{rad}$; (c) after $N = 2$ revolutions; and (d) the time after which it stops.
Explanation of Method
Angular velocity after a time, an angle and two revolutions.
Step 1: Accelerating or decelerating?
Part (d) asks when the body stops, so the angular acceleration must slow it down: $\alpha = -0.5\ \mathrm{rad/s^2}$. The formulas are
\[ \omega = \omega_0 - |\alpha|\,t, \]
\[ \omega^2 = \omega_0^2 - 2|\alpha|\,\theta. \]
Step 2: (a) After 1 s
\[ \omega = 4 - 0.5 \cdot 1. \]
\[\omega = 3.5\ \mathrm{rad/s}\]
Step 3: (b) After $\pi/3$ rad
\[ \omega = \sqrt{16 - 2 \cdot 0.5 \cdot \tfrac{\pi}{3}} = \sqrt{16 - 1.047}. \]
\[\omega \approx 3.87\ \mathrm{rad/s}\]
Step 4: (c) After 2 revolutions
Two revolutions are $4\pi \approx 12.57\ \mathrm{rad}$. The body can turn through $\tfrac{\omega_0^2}{2|\alpha|} = 16\ \mathrm{rad}$ (about 2.5 revolutions) before stopping, so it does complete 2 revolutions:
\[ \omega = \sqrt{16 - 2 \cdot 0.5 \cdot 4\pi} = \sqrt{16 - 12.57}. \]
\[\omega \approx 1.85\ \mathrm{rad/s}\]
Step 5: (d) Time to stop
\[ 0 = 4 - 0.5\,t. \]
\[t = 8\ \mathrm{s}\]
Result
\[\boxed{\,\omega = 3.5\ \mathrm{rad/s}\,}\]
\[\boxed{\,\omega \approx 3.87\ \mathrm{rad/s}\,}\]
\[\boxed{\,\omega \approx 1.85\ \mathrm{rad/s}\,}\]
\[\boxed{\,t = 8\ \mathrm{s}\,}\]
Remark
About the original solution. It used $+0.5\ \mathrm{rad/s^2}$ (speeding up) in parts (a)–(c) but $-0.5$ in part (d), which is inconsistent: a body that speeds up never stops. With the speeding-up reading, the answers to (a)–(c) would be 4.5, 4.13 and 5.34 rad/s, and part (d) would have no answer. The decelerating reading above is the only one that fits all four parts.