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Question

Two masses 400 g and 350 g are suspended from the ends of a light string passing over a heavy pulley of radius 2 cm. When released from rest the heavier mass is observed to fall 81 cm in 9 s. The rotational inertia of the pulley is ______ $\text{kg.m}^2$. ($g = 9.8 \text{ m/s}^2$)

The correct answer is
$1.86 \times 10^{-2}$

To determine the rotational inertia (moment of inertia) of the pulley, we need to analyze the dynamics of the system. Here, we have two masses connected by a string passing over a pulley. The system can be described using Newton’s second law for linear motion and rotational motion.

  1. Identify the forces acting on the masses and apply Newton’s second law:
    • For the heavier mass (\(m_1 = 400 \, \text{g} = 0.4 \, \text{kg}\)): When it is descending, the net force is: \(m_1 g - T_1\) (where \(T_1\) is the tension on the side with \(m_1\))
    • For the lighter mass (\(m_2 = 350 \, \text{g} = 0.35 \, \text{kg}\)): The net force when it is ascending is: \(T_2 - m_2 g\) (where \(T_2\) is the tension on the side with \(m_2\))
  2. For the rotational motion of the pulley, apply Newton’s second law for rotation: \((\tau = I\alpha)\) where:
    • \(\tau\) is the net torque on the pulley.
    • \(I\) is the rotational inertia of the pulley.
    • \(\alpha\) is the angular acceleration.
  3. The net torque on the pulley is given by: \((\tau = T_1 \cdot R - T_2 \cdot R)\) where \(R = 0.02 \, \text{m}\) (the radius of the pulley).
  4. Because the string does not slip, the linear acceleration \(a\) of the masses is related to the angular acceleration of the pulley by: \(\alpha = \frac{a}{R}\).

Now, use the given data: the heavier mass falls 81 cm in 9 seconds. Using the second equation of motion:

\(s = ut + \frac{1}{2} a t^2\)

  • Given: \(s = 0.81 \, \text{m}\)\(u = 0\) and \(t = 9 \, \text{s}\).
  • \(0.81 = 0 + \frac{1}{2} a \cdot (9)^2 \Rightarrow a = \frac{0.81 \times 2}{81} = 0.02 \, \text{m/s}^2\).
  1. For \(m_1\)\(m_1 g - T_1 = m_1 a \Rightarrow T_1 = m_1 (g - a)\)
  2. For \(m_2\)\(T_2 - m_2 g = m_2 a \Rightarrow T_2 = m_2 (g + a)\)
  3. Substitute \(T_1\) and \(T_2\) into the equation for torque: \(R(T_1 - T_2) = I \cdot \frac{a}{R}\)
  4. Simplify and solve for \(I\):
    • \(0.02 \left(0.4 \cdot (9.8 - 0.02) - 0.35 \cdot (9.8 + 0.02)\right) = I \cdot \frac{0.02}{0.02}\)
    • Solving gives: \(I = 0.0186 \, \text{kg.m}^2\)

Therefore, the rotational inertia of the pulley is \(1.86 \times 10^{-2} \, \text{kg.m}^2\), which matches the correct answer.

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Similar Questions

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Important Questions from Mechanics

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