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Power transfer and pf of motor on infinite bus

Short answer

With Ef = 1.5∠120° pu, power transfer = 1.443 pu = 14.43 MW delivered to bus (generating); power factor = 0.596 leading. If Ef angle is -120°, motor absorbs 14.43 MW at 0.596 lagging.

A 3 phase, 10 MVA, 2300 V, 60 Hz synchronous motor has Xs = 0.9 pu and negligible stator resistance. The motor is connected to infinite bus. If terminal voltage, Vt = 2300∠0 V and excitation emf Ef = 3450∠120 V [printed "3450V<120"]. Determine power transfer and power factor of machine. Also draw phasor diagram.

Reading of data: Vt=2300V_t = 2300 V and Ef=3450E_f = 3450 V are taken as line values (the rating is 2300 V line), with EfE_f at +120∘+120^\circ as printed. Work in per unit on 10 MVA, 2300 V.

Vt=23002300=1∠0∘ pu,Ef=34502300∠120∘=1.5∠120∘=−0.75+j1.299 puZbase=2300210×106=0.529 Ω,Xs=0.9×0.529=0.4761 ΩIbase=10×1063×2300=2510.2 A\begin{aligned} V_t &= \frac{2300}{2300} = 1\angle0^\circ\ \text{pu},\quad E_f = \frac{3450}{2300}\angle120^\circ = 1.5\angle120^\circ = -0.75 + j1.299\ \text{pu} \\ Z_{base} &= \frac{2300^2}{10\times10^6} = 0.529\ \Omega,\quad X_s = 0.9 \times 0.529 = 0.4761\ \Omega \\ I_{base} &= \frac{10\times10^6}{\sqrt3 \times 2300} = 2510.2\ \text{A} \end{aligned}

Power transfer

P=VtEfXssin⁡δ=1×1.50.9sin⁡120∘=1.4434 pu=14.43 MWP = \frac{V_tE_f}{X_s}\sin\delta = \frac{1 \times 1.5}{0.9}\sin120^\circ = 1.4434\ \text{pu} = 14.43\ \text{MW}

Current and power factor

Using the motor equation V⃗t=E⃗f+jXsI⃗a\vec V_t = \vec E_f + jX_s\vec I_a:

I⃗a=V⃗t−E⃗fjXs=1.75−j1.299j0.9=−1.4434−j1.9444=2.4216∠−126.59∘ pu=6079 AS⃗=V⃗tI⃗a∗=−1.4434+j1.9444 pu\begin{aligned} \vec I_a &= \frac{\vec V_t - \vec E_f}{jX_s} = \frac{1.75 - j1.299}{j0.9} = -1.4434 - j1.9444 \\ &= 2.4216\angle -126.59^\circ\ \text{pu} = 6079\ \text{A} \\ \vec S &= \vec V_t\vec I_a^{*} = -1.4434 + j1.9444\ \text{pu} \end{aligned}

The real part is negative: since EfE_f leads VtV_t, the machine is not taking power; it is delivering 14.43 MW to the bus, i.e. acting as a generator. Taking the generated current −I⃗a=2.4216∠53.41∘-\vec I_a = 2.4216\angle 53.41^\circ pu, it leads VtV_t by 53.41∘53.41^\circ:

pf=cos⁡53.41∘=0.596 leading\text{pf} = \cos53.41^\circ = 0.596\ \text{leading}
        Ef (1.5 pu)
          \
           \ at 120 deg from Vt
            \
             O-----------> Vt (1.0 pu)
              \
               \  Ia (motor convention)
                v at -126.6 deg
 jXs.Ia = Vt - Ef joins tip of Ef to tip of Vt
 Ia(gen) = -Ia leads Vt by 53.4 deg

Note: with δ=120∘\delta = 120^\circ the machine is beyond the steady-state limit (90∘90^\circ) and the current (2.42 pu) is far above rating, so this point is not a stable working point. If the angle was meant as −120∘-120^\circ (motor action, EfE_f lagging), the same magnitudes result: the motor absorbs 14.43 MW at a pf of 0.596 lagging.

Answer: Power transferred =1.443= 1.443 pu =14.43= 14.43 MW; power factor =0.596= 0.596 (leading as printed, i.e. generating; lagging if EfE_f is at −120∘-120^\circ).

✓ Answer checked by Claude Sonnet 5.5

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