Step 1 — New Back-EMF (field reversed)
Reversing the field polarity reverses the back-EMF: \(E_g = -191.4\,\text{V}\).
Armature current direction is unchanged: \(I_a = +38\,\text{A}\).
Step 2 — Required Terminal Voltage
\[
V_a = E_g + I_a R_a = -191.4 + 38 \times 0.3 = -180.0\,\text{V}
\]
Step 3 — Firing Angle for Inverter Mode
\[
\cos\alpha = \frac{V_a \cdot \pi}{2\sqrt{2}\,V_s}
= \frac{-180.0\,\pi}{2\sqrt{2} \times 260} = -0.769
\]
\[
\alpha = \cos^{-1}(-0.769) = \mathbf{140.3°}
\]
Note: \(\alpha > 90°\) confirms inverter (regenerating) operation.
Step 4 — Power Fed Back to Supply
\[
P_g = |E_g| \cdot I_a = 191.4 \times 38 = 7273\,\text{W}
\]
\[
P_R = I_a^2 R_a = 38^2 \times 0.3 = 433\,\text{W}
\]
\[
P_s = P_g - P_R = 7273 - 433 = \mathbf{6840\,\text{W}}
\]
Part 2 — Results Summary
| Quantity | Value |
| Firing angle \(\alpha\) | 140.3° |
| Power fed back \(P_s\) | 6840 W |
Inverter Mode — Physical Explanation
During regenerative braking, the motor acts as a generator. The back-EMF drives current through the armature in the same direction as before, but the terminal voltage is now negative. The converter fires late (\(\alpha > 90°\)) so its average output opposes the back-EMF, channelling motor kinetic energy back to the AC supply. Armature copper loss \((P_R = 433\,\text{W})\) is the only energy not returned.