Step 1: Use the equation for angular velocity.
We are given that the initial angular speed is 800 rpm and the final angular speed is 2100 rpm.
The equation for angular velocity is given by:
\[
\omega_f = \omega_i + \alpha t
\]
where \( \omega_f \) is the final angular velocity, \( \omega_i \) is the initial angular velocity, \( \alpha \) is the angular acceleration, and \( t \) is the time.
Converting rpm to rad/s:
\[
\omega_i = 800 \times \frac{2\pi}{60} = \frac{16\pi}{3} \, \text{rad/s}, \quad \omega_f = 2100 \times \frac{2\pi}{60} = 35\pi \, \text{rad/s}
\]
Now, substitute the values into the equation:
\[
35\pi = \frac{16\pi}{3} + \alpha \times 40
\]
Solving for \( \alpha \):
\[
\alpha = \frac{13\pi}{12} \, \text{rad/s}^2
\]
Step 2: Use the equation for torque.
We are given a torque of \( \tau = 25\pi \, \text{Nm} \).
The torque is related to the angular acceleration and moment of inertia \( I \) by:
\[
\tau = I \alpha
\]
For a disc rotating about its diameter, the moment of inertia is:
\[
I = \frac{1}{4} m r^2
\]
Substitute the values into the torque equation:
\[
25\pi = \frac{1}{4} m r^2 \times \frac{13\pi}{12}
\]
Simplifying:
\[
\frac{25\pi}{13\pi} = \frac{m r^2}{4 \times 12}
\]
\[
\frac{25}{13} = \frac{m r^2}{48}
\]
Since \( m = 1 \, \text{kg} \), this simplifies to:
\[
\frac{25}{13} = \frac{r^2}{48}
\]
Solving for \( r^2 \):
\[
r^2 = \frac{25 \times 48}{13} = \frac{1200}{13}
\]
\[
r = \sqrt{\frac{1200}{13}} \approx 10.53 \, \text{m}
\]
Step 3: Calculate the Diameter.
The diameter \( D \) is twice the radius:
\[
D = 2r = 2 \times 10.53 \approx 20.87 \, \text{m}
\]
Thus, the correct answer is \( \boxed{40 \sqrt{\frac{3}{13}}} \).