A thin solid disk of $1$ kg is rotating along its diameter axis at the speed of $1800$ rpm. By applying an external torque of $25\pi$ Nm for $40$ s, the speed increases to $2100$ rpm. The diameter of the disk is ____ m.
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Solution Steps
1
Convert Speeds to Angular Velocity ($\omega$)
Initial angular velocity, $\omega_i = 1800 \text{ rpm} = \frac{1800 \times 2\pi}{60} = 60\pi \text{ rad/s}$.
Final angular velocity, $\omega_f = 2100 \text{ rpm} = \frac{2100 \times 2\pi}{60} = 70\pi \text{ rad/s}$.
2
Calculate Angular Acceleration ($\alpha$)
Using the kinematic equation $\omega_f = \omega_i + \alpha t$:
$$70\pi = 60\pi + \alpha(40)$$
$$10\pi = 40\alpha \implies \alpha = \frac{\pi}{4} \text{ rad/s}^2$$
3
Relate Torque to Moment of Inertia
Using $\tau = I\alpha$, where $\tau = 25\pi$ Nm:
$$25\pi = I \left(\frac{\pi}{4}\right)$$
$$I = 25 \times 4 = 100 \text{ kg}\cdot\text{m}^2$$
4
Find Radius using Moment of Inertia Formula
For a disk about its diameter, $I = \frac{1}{4}MR^2$. Given $M = 1$ kg:
$$100 = \frac{1}{4}(1)R^2 \implies R^2 = 400$$
$$R = \sqrt{400} = 20 \text{ m}$$
5
Calculate Diameter
Diameter $D = 2R = 2 \times 20 = 40$ m.
Final Answer: 40
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Theory
1. Moment of Inertia of a Disk
The moment of inertia (MOI) represents an object’s resistance to rotational acceleration. For a uniform thin solid disk of mass $M$ and radius $R$, the MOI depends on the axis of rotation. About the central longitudinal axis (perpendicular to the plane), $I = \frac{1}{2}MR^2$. However, about any diameter axis (lying in the plane of the disk), we apply the Perpendicular Axis Theorem ($I_z = I_x + I_y$), which yields $I_{dia} = \frac{1}{4}MR^2$. Understanding the specific axis is critical for JEE problems.
2. Rotational Kinematics
Rotational kinematics describes the motion of rotating objects using angular displacement ($\theta$), angular velocity ($\omega$), and angular acceleration ($\alpha$). These variables are analogous to linear displacement, velocity, and acceleration. Under constant torque, the angular acceleration is constant, allowing the use of equations like $\omega_f = \omega_i + \alpha t$ and $\theta = \omega_i t + \frac{1}{2}\alpha t^2$. Always ensure angular velocity is converted from RPM to rad/s ($1 \text{ rpm} = \pi/30 \text{ rad/s}$) for SI consistency.
3. Torque and Newton’s Second Law
Torque ($\tau$) is the rotational equivalent of force. According to Newton’s Second Law for rotation, the net external torque applied to a rigid body is equal to the product of its moment of inertia and its angular acceleration ($\tau = I\alpha$). This relationship is valid when $I$ is measured about the same axis as the torque. In this problem, a constant torque over a period of time causes a linear change in the angular momentum and angular velocity of the disk.
4. Work and Energy in Rotation
Applying torque over an angular displacement results in work done: $W = \tau \theta$. This work increases the rotational kinetic energy of the system, given by $K_{rot} = \frac{1}{2}I\omega^2$. The Work-Energy Theorem for rotation states that the net work done by external torques equals the change in rotational kinetic energy. While not directly required to find the diameter here, energy methods are often faster alternatives for complex JEE problems involving varying torques or speeds.
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FAQs
1
Why did we use $I = \frac{1}{4}MR^2$?
Because the problem specifies the rotation is “along its diameter axis” rather than its center perpendicular axis.
2
How do I convert 1800 rpm to rad/s?
$\omega = \frac{1800 \times 2\pi}{60} = 30 \times 2\pi = 60\pi \text{ rad/s}$.
3
What if the disk was a ring?
For a ring about its diameter, $I = \frac{1}{2}MR^2$. The resulting diameter would be different.
4
Is the “thin” disk assumption important?
Yes, “thin” implies we can treat it as a 2D object and ignore the height (thickness) in MOI calculations.
5
What is the value of $\alpha$ in this question?
The angular acceleration $\alpha$ is $\pi/4$ rad/s².
6
Can the diameter be negative?
No, diameter is a physical length and must be positive ($+40$ m).
7
What is the SI unit of Moment of Inertia?
The unit is $\text{kg}\cdot\text{m}^2$.
8
Does the time (40s) affect the MOI?
No, MOI is a property of mass distribution; time only affects how much the speed changes for a given torque.
9
What if torque was not constant?
Then $\alpha$ would vary, and we would need to use integration: $\int \tau dt = I(\omega_f – \omega_i)$.
10
How do I calculate $\pi$ in the final answer?
Notice that $\pi$ cancels out during the $\tau = I\alpha$ calculation, leaving a purely numerical result.
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