To determine the angular acceleration produced in the hollow cylinder when the rope is pulled with a force, we begin by analyzing the situation using the following physics principles:
1. **Understand the Concept**: The problem involves a force applied to a cylindrical object causing it to rotate. The angular acceleration can be calculated using the relation between torque, moment of inertia, and angular acceleration.
2. **Identify Given Values**:
3. **Formula for Torque**: Torque (\tau) can be computed using the formula:
\tau = F \cdot r
Substituting the given values:
\tau = 30 \, \text{N} \times 0.4 \, \text{m} = 12 \, \text{Nm}
4. **Moment of Inertia for a Hollow Cylinder**: The moment of inertia (I) for a hollow cylinder about its central axis is given by:
I = m \cdot r^2
Substituting the known values:
I = 3 \, \text{kg} \times (0.4 \, \text{m})^2 = 0.48 \, \text{kg} \, \text{m}^2
5. **Calculating Angular Acceleration**: Using the relation between torque and angular acceleration (\alpha):
\tau = I \cdot \alpha
Substituting for torque and moment of inertia:
12 \, \text{Nm} = 0.48 \, \text{kg} \, \text{m}^2 \times \alpha
Solving for \alpha:
\alpha = \frac{12 \, \text{Nm}}{0.48 \, \text{kg} \, \text{m}^2} = 25 \, \text{rad} \, \text{s}^{-2}
Hence, the angular acceleration produced in the cylinder is 25 \, \text{rad} \, \text{s}^{-2}. Therefore, the correct answer is the option:
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 