To find the angular acceleration \( \alpha \), we use the relation between torque \( \tau \), moment of inertia \( I \), and angular acceleration:
\[\tau = I \cdot \alpha\]
The torque \( \tau \) is given by the product of the applied force \( F \) and the radius \( r \) of the disk:
\[\tau = F \cdot r\]
Substitute the given values: \( F = 15 \, \text{N} \), \( r = 0.1 \, \text{m} \), and \( I = 0.02 \, \text{kg} \cdot \text{m}^2 \).
Calculate the torque:
\[\tau = 15 \, \text{N} \times 0.1 \, \text{m} = 1.5 \, \text{Nm}\]
Now, substitute \( \tau \) into the first equation to solve for \( \alpha \):
\[1.5 = 0.02 \cdot \alpha\]
Solve for \( \alpha \):
\[\alpha = \frac{1.5}{0.02} = 75 \, \text{rad/s}^2\]
The angular acceleration \( \alpha \) is 75 rad/s\(^2\).