Let:
- Initial speed = \( N \), new speed = \( N/2 \)
- Torque \( T \propto N^3 \Rightarrow T_2 = \left(\frac{N}{2}\right)^3 = \frac{1}{8} T_1 \)
For a DC series motor with negligible internal resistance and assuming a linear magnetic circuit:
- Torque \( T \propto \phi I \propto I^2 \Rightarrow T \propto I^2 \)
- So \( \frac{T_2}{T_1} = \left( \frac{I_2}{I_1} \right)^2 = \frac{1}{8} \Rightarrow I_2 = \frac{I_1}{\sqrt{8}} = \frac{40}{\sqrt{8}} = 14.14 \, {A} \)
Now, for a DC motor:
- \( V = E + I_a R \), and for negligible resistance, initially:
\[ E_1 = V = 400 \, {V} \]
Back EMF is proportional to speed and flux:
\[ E \propto N \phi \Rightarrow E_2 = \frac{1}{2} \cdot \frac{14.14}{40} \cdot E_1 = \frac{1}{2} \cdot \frac{14.14}{40} \cdot 400 = 70.7 \, {V} \]
Now apply KVL with external resistance \( R \):
\[ V = E_2 + I_2 R \Rightarrow 400 = 70.7 + 14.14 R \]
