Assuming the input power and terminal voltage for the motor of Example 5.1 remain constant, calculate (a) the phase angle δ of the generated voltage and (b) the field current required to achieve unity power factor at the motor terminals.
a. For unity power factor at the motor terminals, the phase-a terminal current will be in phase with the phase-a line-to-neutral voltage \hat{V}_a. Thus
\hat{I}_a=\frac{P_{in}}{3V_a} = \frac{90.6 kW}{3×265.6 V} = 114 A
From Eq. 5.23,
\hat{V}_a=R_a \hat{I}_a+ jX_s \hat{I}_a+ \hat{E}_{af} (5.23)
\begin{aligned}\hat{E}_{af}&= \hat{V}_a – jX_s\hat{I}_a \\&= 265.6 – j 1.68 × 114 = 328 e^{- j35.8°} V,\text{ line-to-neutral}\end{aligned}
Thus, E_{af} = 328 V line-to-neutral and δ = -35.8° .
b. Having found L_{af} in Example 5.1, we can find the required field current from Eq. 5.21.
E_{af}=\frac{ω_e L_{af}I_f}{\sqrt{2}} (5.21)
I_f = \frac{\sqrt{2}E_{af}}{ω_e L_{af}} =\frac{\sqrt{2} × 328}{377× 0.0223}= 55.2 A