Math Problem Statement

A uniform disk with radius R = 0.400 m is mounted on a horizontal frictionless axle at its center. A light string is wrapped around the disk. The disk is initially at rest and then a constant force of 6.00 N is applied to the free end of the rope. After the force has been applied for 4.00 s, the disk is rotating with angular velocity 12.0 rad/s. What is the mass of the disk?

Solution

To solve this problem, let’s break down the information provided:

Given Data:

  1. Radius of the disk: R=0.400mR = 0.400 \, \text{m}
  2. Force applied: F=6.00NF = 6.00 \, \text{N}
  3. Time duration: t=4.00st = 4.00 \, \text{s}
  4. Final angular velocity: ω=12.0rad/s\omega = 12.0 \, \text{rad/s}
  5. Moment of inertia of a uniform disk: I=12mR2I = \frac{1}{2} m R^2

Steps to Solve:

  1. Calculate the Torque (τ\tau):

    • Torque is given by τ=FR\tau = F \cdot R.
    • Substitute F=6.00NF = 6.00 \, \text{N} and R=0.400mR = 0.400 \, \text{m}: τ=6.00×0.400=2.4Nm\tau = 6.00 \times 0.400 = 2.4 \, \text{Nm}
  2. Calculate Angular Acceleration (α\alpha):

    • Torque is also related to angular acceleration by τ=Iα\tau = I \alpha.
    • Substitute I=12mR2I = \frac{1}{2} m R^2: τ=12mR2α\tau = \frac{1}{2} m R^2 \cdot \alpha
    • Solving for α\alpha: α=2τmR2\alpha = \frac{2 \tau}{m R^2}
  3. Relate Angular Acceleration and Final Angular Velocity:

    • Using ω=αt\omega = \alpha t to find α\alpha: α=ωt=12.04.0=3.0rad/s2\alpha = \frac{\omega}{t} = \frac{12.0}{4.0} = 3.0 \, \text{rad/s}^2
  4. Solve for the Mass mm:

    • Substitute α=3.0rad/s2\alpha = 3.0 \, \text{rad/s}^2 and τ=2.4Nm\tau = 2.4 \, \text{Nm}: 2.4=12m(0.4)23.02.4 = \frac{1}{2} m (0.4)^2 \cdot 3.0 m=2.40.24=10.0kgm = \frac{2.4}{0.24} = 10.0 \, \text{kg}

Answer:

The mass of the disk is 10.0 kg (Option C).

Would you like further explanation on any of the steps or have additional questions?


Additional Questions:

  1. What is the relationship between torque and angular acceleration?
  2. How would the mass change if the applied force were different?
  3. What would be the effect of a larger radius on the angular acceleration?
  4. How does the time duration affect the final angular velocity?
  5. Why is the moment of inertia different for various shapes?

Tip:

Remember, torque and force are related but act differently in rotational and linear dynamics.

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Math Problem Analysis

Mathematical Concepts

Physics
Rotational Dynamics
Torque
Angular Acceleration
Moment of Inertia

Formulas

Torque (τ) = Force (F) * Radius (R)
Moment of Inertia (I) for a disk = (1/2) * m * R^2
Torque (τ) = I * Angular Acceleration (α)
Angular Velocity (ω) = α * Time (t)

Theorems

Newton's Second Law for Rotation

Suitable Grade Level

Undergraduate Physics