Step 1: Determine angular acceleration.
The initial angular speed is 800 rpm, and the final angular speed is 2100 rpm. The equation for angular velocity is \( \omega_f = \omega_i + \alpha t \).
Convert rpm to rad/s:
\[\omega_i = 800 \times \frac{2\pi}{60} = \frac{16\pi}{3} \, \text{rad/s}, \quad \omega_f = 2100 \times \frac{2\pi}{60} = 35\pi \, \text{rad/s}\]
Substitute known values into the angular velocity equation:\[35\pi = \frac{16\pi}{3} + \alpha \times 40\]
Solve for angular acceleration \( \alpha \):\[\alpha = \frac{13\pi}{12} \, \text{rad/s}^2\]
Step 2: Calculate the moment of inertia.
A torque of \( \tau = 25\pi \, \text{Nm} \) is applied. The relationship between torque, moment of inertia \( I \), and angular acceleration is \( \tau = I \alpha \).
For a disc rotating about its diameter, the moment of inertia is \( I = \frac{1}{4} m r^2 \).
Substitute values into the torque equation:\[25\pi = \frac{1}{4} m r^2 \times \frac{13\pi}{12}\]
Simplify the equation:\[\frac{25}{13} = \frac{m r^2}{48}\]
Given that mass \( m = 1 \, \text{kg} \), the equation becomes:\[\frac{25}{13} = \frac{r^2}{48}\]
Solve for \( r^2 \):\[r^2 = \frac{25 \times 48}{13} = \frac{1200}{13}\]
Calculate the radius \( r \):\[r = \sqrt{\frac{1200}{13}} \approx 10.53 \, \text{m}\]
Step 3: Compute the Diameter.
The diameter \( D \) is twice the radius:\[D = 2r = 2 \times 10.53 \approx 20.87 \, \text{m}\]
The correct answer is \( \boxed{40 \sqrt{\frac{3}{13}}} \).