Given the conditions of the problem, we know that the flywheels are connected by a non-slipping belt. Therefore, the angular acceleration of the smaller wheel (\( \alpha_1 \)) and the larger wheel (\( \alpha_2 \)) are related by the following equation:
\[
\alpha_1 r_1 = \alpha_2 r_2
\]
where \( r_1 \) and \( r_2 \) are the radii of the smaller and larger wheels, respectively.
1. Angular acceleration of the smaller wheel (\( \alpha_1 \)):
The angular acceleration of the smaller wheel is determined from the applied torque \( \tau_1 \) using the relation:
\[
\tau_1 = I_1 \alpha_1
\]
where \( I_1 \) is the moment of inertia of the smaller wheel, given by \( I_1 = \frac{1}{2} m_1 r_1^2 \). Thus:
\[
I_1 = \frac{1}{2} \times 4 \, \text{kg} \times (0.2 \, \text{m})^2 = 0.08 \, \text{kg} \, \text{m}^2
\]
The torque applied is \( \tau_1 = 10 \, \text{Nm} \), so:
\[
\alpha_1 = \frac{\tau_1}{I_1} = \frac{10}{0.08} = 125 \, \text{rad/s}^2
\]
2. Angular acceleration of the larger wheel (\( \alpha_2 \)):
Using the relationship \( \alpha_1 r_1 = \alpha_2 r_2 \), we can find \( \alpha_2 \):
\[
\alpha_2 = \frac{\alpha_1 r_1}{r_2} = \frac{125 \times 0.2}{0.3} = 83.33 \, \text{rad/s}^2
\]
3. Torque on the larger wheel (\( \tau_2 \)):
The torque on the larger wheel is given by:
\[
\tau_2 = I_2 \alpha_2
\]
where \( I_2 = \frac{1}{2} m_2 r_2^2 \). Thus:
\[
I_2 = \frac{1}{2} \times 20 \, \text{kg} \times (0.3 \, \text{m})^2 = 0.9 \, \text{kg} \, \text{m}^2
\]
Therefore:
\[
\tau_2 = 0.9 \times 83.33 = 75 \, \text{Nm}
\]
Thus, the numerical values corresponding to the quantities are:
- \( \alpha_1 = 125 \, \text{rad/s}^2 \) (which matches option iii),
- \( \tau_2 = 75 \, \text{Nm} \) (which matches option ii),
- \( \alpha_2 = 83.33 \, \text{rad/s}^2 \) (which matches option i).