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A solid cylinder of mass 2 kg and radius...

A solid cylinder of mass 2 kg and radius 4 cm rotating about its axis at the rate of 3 rpm. The torque required to stop after `2pi` revolutions is :

A

`2xx10^(6)Nm`

B

`2xx10^(-6)Nm`

C

`2xx10^(-3)Nm`

D

`12xx10^(-4)Nm`

Text Solution

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The correct Answer is:
To solve the problem, we need to calculate the torque required to stop a solid cylinder that is rotating. Here’s a step-by-step solution: ### Step 1: Convert the rotation speed from rpm to rad/s The cylinder is rotating at 3 revolutions per minute (rpm). We need to convert this to radians per second. \[ \text{Angular velocity} \, (\omega) = 3 \, \text{rpm} \times \frac{2\pi \, \text{radians}}{1 \, \text{revolution}} \times \frac{1 \, \text{minute}}{60 \, \text{seconds}} \] Calculating this gives: \[ \omega = 3 \times \frac{2\pi}{60} = \frac{6\pi}{60} = \frac{\pi}{10} \, \text{rad/s} \] ### Step 2: Calculate the total angle in radians for 2π revolutions The cylinder needs to stop after 2π revolutions. We convert this to radians: \[ \theta = 2\pi \, \text{revolutions} \times 2\pi \, \text{radians/revolution} = 4\pi^2 \, \text{radians} \] ### Step 3: Use the angular kinematic equation to find angular acceleration (α) We can use the equation: \[ \omega^2 = \omega_0^2 + 2\alpha\theta \] Where: - \(\omega = 0\) (final angular velocity since the cylinder stops) - \(\omega_0 = \frac{\pi}{10}\) (initial angular velocity) - \(\theta = 4\pi^2\) (total angle in radians) Substituting the values: \[ 0 = \left(\frac{\pi}{10}\right)^2 + 2\alpha(4\pi^2) \] This simplifies to: \[ 0 = \frac{\pi^2}{100} + 8\pi^2\alpha \] Rearranging gives: \[ 8\pi^2\alpha = -\frac{\pi^2}{100} \] Dividing both sides by \(8\pi^2\): \[ \alpha = -\frac{1}{800} \, \text{rad/s}^2 \] ### Step 4: Calculate the moment of inertia (I) of the solid cylinder The moment of inertia of a solid cylinder about its axis is given by: \[ I = \frac{1}{2} m r^2 \] Where: - \(m = 2 \, \text{kg}\) - \(r = 4 \, \text{cm} = 0.04 \, \text{m}\) Calculating \(I\): \[ I = \frac{1}{2} \times 2 \times (0.04)^2 = \frac{1}{2} \times 2 \times 0.0016 = 0.0016 \, \text{kg m}^2 \] ### Step 5: Calculate the torque (τ) Torque is given by the formula: \[ \tau = I \alpha \] Substituting the values we have: \[ \tau = 0.0016 \times \left(-\frac{1}{800}\right) \] Calculating this gives: \[ \tau = -\frac{0.0016}{800} = -2 \times 10^{-6} \, \text{N m} \] Since we are interested in the magnitude of torque, we can state: \[ \tau = 2 \times 10^{-6} \, \text{N m} \] ### Final Answer The torque required to stop the cylinder after \(2\pi\) revolutions is: \[ \boxed{2 \times 10^{-6} \, \text{N m}} \]

To solve the problem, we need to calculate the torque required to stop a solid cylinder that is rotating. Here’s a step-by-step solution: ### Step 1: Convert the rotation speed from rpm to rad/s The cylinder is rotating at 3 revolutions per minute (rpm). We need to convert this to radians per second. \[ \text{Angular velocity} \, (\omega) = 3 \, \text{rpm} \times \frac{2\pi \, \text{radians}}{1 \, \text{revolution}} \times \frac{1 \, \text{minute}}{60 \, \text{seconds}} \] ...
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Knowledge Check

  • A solid sphere of mass 2 kg and radius 5 cm is rotating at the rate of 300 rpm. The torque required to stop it in 2pi revolutions is

    A
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    B
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    C
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    D
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    A
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    B
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    C
    if a retarding torque of 200N-m starts acting then it will come at rest after 5 sec.
    D
    all of these
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    A
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    B
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    C
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    D
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