Question:

$A$ uniform rod of length $200\, cm$ and mass $500\, g$ is balanced on a wedge placed at $40\, cm$ mark. A mass of $2\, kg$ is suspended from the rod at $20\, cm$ and another unknown mass ' $m$ ' is suspended from the rod at $160\, cm$ mark as shown in the figure Find the value of 'm' such that the rod is in equilibrium. $\left( g =10\, m / s ^{2}\right)$

Updated On: Nov 13, 2025
  • $\frac{1}{2} kg$
  • $\frac{1}{3} kg$
  • $\frac{1}{6} kg$
  • $\frac{1}{12} kg$
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The Correct Option is D

Solution and Explanation

To solve this problem, we need to ensure that the rod is in rotational equilibrium. Therefore, the sum of the torques around the pivot point (the wedge at the 40 cm mark) must be zero.

Let's analyze the situation: 

  • The length of the rod is \(200 \, \text{cm}\), and its center of mass is at the \(100 \, \text{cm}\) mark.
  • The rod's mass is \(500 \, \text{g} = 0.5 \, \text{kg}\). Thus, its weight is \(0.5 \, \text{kg} \times 10 \, \text{m/s}^2 = 5 \, \text{N}\).
  • A mass of \(2 \, \text{kg}\) is suspended at the \(20 \, \text{cm}\) mark, creating a force of \(2 \, \text{kg} \times 10 \, \text{m/s}^2 = 20 \, \text{N}\).
  • An unknown mass \(m\) is suspended at the \(160 \, \text{cm}\) mark.

We will calculate the torques around the pivot point (\(40 \, \text{cm}\) mark). The torque \((\tau)\) caused by a force \((F)\) at a distance \((d)\) from the pivot is given by:

\(\tau = F \times d\)

Let's calculate the torque for each force:

  1. Torque due to the 2 kg mass at 20 cm mark:
    • Distance from pivot = \(40 \, \text{cm} - 20 \, \text{cm} = 20 \, \text{cm} = 0.2 \, \text{m}\)
    • Torque = \(20 \, \text{N} \times 0.2 \, \text{m} = 4 \, \text{Nm}\) (Clockwise)
  2. Torque due to the rod's weight:
    • Distance from pivot = \(100 \, \text{cm} - 40 \, \text{cm} = 60 \, \text{cm} = 0.6 \, \text{m}\)
    • Torque = \(5 \, \text{N} \times 0.6 \, \text{m} = 3 \, \text{Nm}\) (Anticlockwise)
  3. Torque due to the unknown mass \(m\) at 160 cm mark:
    • Distance from pivot = \(160 \, \text{cm} - 40 \, \text{cm} = 120 \, \text{cm} = 1.2 \, \text{m}\)
    • Torque = \(m \times 10 \, \text{m/s}^2 \times 1.2 \, \text{m} = 12m \, \text{Nm}\) (Anticlockwise)

For rotational equilibrium, the sum of the clockwise torques must equal the sum of anticlockwise torques:

\(4 \, \text{Nm} = 3 \, \text{Nm} + 12m \, \text{Nm}\)

Solving for \(m\):

\(4 - 3 = 12m\)

\(1 = 12m\)

\(m = \frac{1}{12} \, \text{kg}\)

Therefore, the mass \(m\) required for the rod to be in equilibrium is \(\frac{1}{12} \, \text{kg}\).

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Concepts Used:

Moment of Inertia

Moment of inertia is defined as the quantity expressed by the body resisting angular acceleration which is the sum of the product of the mass of every particle with its square of a distance from the axis of rotation.

Moment of inertia mainly depends on the following three factors:

  1. The density of the material
  2. Shape and size of the body
  3. Axis of rotation

Formula:

In general form, the moment of inertia can be expressed as, 

I = m × r²

Where, 

I = Moment of inertia. 

m = sum of the product of the mass. 

r = distance from the axis of the rotation. 

M¹ L² T° is the dimensional formula of the moment of inertia. 

The equation for moment of inertia is given by,

I = I = ∑mi ri²

Methods to calculate Moment of Inertia:

To calculate the moment of inertia, we use two important theorems-

  • Perpendicular axis theorem
  • Parallel axis theorem