Question:

An electric motor’s rotor is spinning at 1500 rpm when its load and power are cut off. The rotor, which has a mass of 50 kg and a radius of gyration of 200 mm, then coasts down to rest. Due to kinetic friction, a constant torque of 10 Nm acts on the rotor as it coasts down.
The number of revolutions executed by the rotor before it comes to rest is .......... (in integer).

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For problems involving deceleration due to a constant torque, use the kinematic equation for angular motion: \( \theta = \frac{\omega_0^2}{2\alpha} \), and remember to convert radians to revolutions using \( 2\pi \).
Updated On: May 7, 2025
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Solution and Explanation

Given: 
- Initial angular velocity, \( \omega_0 = 1500 \) rpm = \( \frac{1500 \times 2\pi}{60} \) rad/s = 157.08 rad/s 
- Mass of rotor, \( m = 50 \, {kg} \) 
- Radius of gyration, \( k = 0.2 \, {m} \) 
- Torque due to friction, \( \tau = 10 \, {Nm} \) 
Step 1: Moment of Inertia 
The moment of inertia \( I \) of the rotor is given by: 
\[ I = m k^2 = 50 \times (0.2)^2 = 50 \times 0.04 = 2 \, {kg} \cdot {m}^2 \] 
Step 2: Angular Deceleration 
Using the equation for torque, we can find the angular acceleration: 
\[ \tau = I \alpha \Rightarrow \alpha = \frac{\tau}{I} = \frac{10}{2} = 5 \, {rad/s}^2 \] This is the angular deceleration as the rotor is slowing down.
Step 3: Number of Revolutions 
The equation for angular displacement \( \theta \) when the object is under constant angular acceleration is: 
\[ \theta = \frac{\omega_0^2}{2\alpha} \] Substituting the values: 
\[ \theta = \frac{(157.08)^2}{2 \times 5} = \frac{24670.22}{10} = 2467.02 \, {rad} \] To convert from radians to revolutions, we divide by \( 2\pi \): 
\[ {Number of revolutions} = \frac{2467.02}{2\pi} \approx 393 \, {revolutions} \] Thus, the number of revolutions executed by the rotor before it comes to rest is approximately \( 393 \) revolutions. 
 

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