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Salient pole motor excitation and reluctance power

Short answer

Per-unit: V=1, Ia=1∠–36.87°. E' = V – jXq Ia gives δ=22.83°, then Ef = 0.728 pu (8.0 kV line). Excitation power 0.353 pu (17.65 MW), saliency power 0.447 pu (22.35 MW). With zero field, max reluctance power 0.625 pu < required 0.8 pu, so motor falls out of step.

Salient pole synchronous motor has reactance Xd = 0.8 pu, Xq = 0.4 pu. It is a 3-phase, 50 MVA, 11 kV, 50 Hz. Motor draws rated current at a supply power factor of 0.8 lagging. Rotational losses are 0.15 pu and armature resistance losses are neglected. a) Calculate the excitation voltage. b) Find the power due to field excitation and that due to the salience of the machine. c) If the field current is zero, will the machine stay in synchronism, explain why?

Work in per unit: V=1∠0∘V = 1\angle0^\circ pu, rated current Ia=1I_a = 1 pu at 0.8 lagging, so I⃗a=1∠−36.87∘=0.8−j0.6\vec I_a = 1\angle -36.87^\circ = 0.8 - j0.6 pu.

Method (two-reaction theory, motor, Ra=0R_a = 0): V⃗=E⃗f+jXdI⃗d+jXqI⃗q\vec V = \vec E_f + jX_d\vec I_d + jX_q\vec I_q.

  1. E⃗′=V⃗−jXqI⃗a\vec E' = \vec V - jX_q\vec I_a gives the direction of EfE_f (the q-axis), so its angle is −δ-\delta.
  2. Angle between IaI_a and the q-axis: ψ=δ−ϕ\psi = \delta - \phi (ϕ\phi positive for lagging, negative for leading); Id=Iasin⁡ψI_d = I_a\sin\psi, Iq=Iacos⁡ψI_q = I_a\cos\psi.
  3. Ef=E′+(Xd−Xq)IdE_f = E' + (X_d - X_q)I_d.

a) Excitation voltage

E⃗′=1−j0.4(0.8−j0.6)=1−0.24−j0.32=0.76−j0.32=0.8246∠−22.83∘ puδ=22.83∘,ψ=22.83∘−36.87∘=−14.04∘Id=1×sin⁡(−14.04∘)=−0.2425 pu,Iq=0.9701 puEf=0.8246+(0.8−0.4)(−0.2425)=0.7276 pu\begin{aligned} \vec E' &= 1 - j0.4(0.8 - j0.6) = 1 - 0.24 - j0.32 \\ &= 0.76 - j0.32 = 0.8246\angle -22.83^\circ\ \text{pu} \\ \delta &= 22.83^\circ,\quad \psi = 22.83^\circ - 36.87^\circ = -14.04^\circ \\ I_d &= 1 \times \sin(-14.04^\circ) = -0.2425\ \text{pu},\quad I_q = 0.9701\ \text{pu} \\ E_f &= 0.8246 + (0.8 - 0.4)(-0.2425) = 0.7276\ \text{pu} \end{aligned}

Ef=0.7276×11=8.00E_f = 0.7276 \times 11 = 8.00 kV (line), i.e. 4.62 kV per phase. Ef<VE_f < V, as expected for an under-excited (lagging) motor.

b) Excitation power and reluctance power

P=EfVXdsin⁡δ⏟excitation+V22(1Xq−1Xd)sin⁡2δ⏟saliencyP = \underbrace{\frac{E_fV}{X_d}\sin\delta}_{\text{excitation}} + \underbrace{\frac{V^2}{2}\left(\frac{1}{X_q}-\frac{1}{X_d}\right)\sin2\delta}_{\text{saliency}} Pexc=0.7276×10.8sin⁡22.83∘=0.3529 pu=17.65 MWPrel=12(2.5−1.25)sin⁡45.67∘=0.4471 pu=22.35 MWP=0.3529+0.4471=0.8 pu=40 MW\begin{aligned} P_{exc} &= \frac{0.7276 \times 1}{0.8}\sin22.83^\circ = 0.3529\ \text{pu} = 17.65\ \text{MW} \\ P_{rel} &= \frac{1}{2}(2.5 - 1.25)\sin45.67^\circ = 0.4471\ \text{pu} = 22.35\ \text{MW} \\ P &= 0.3529 + 0.4471 = 0.8\ \text{pu} = 40\ \text{MW} \end{aligned}

Check: input =VIcos⁡ϕ=1×1×0.8=0.8= VI\cos\phi = 1 \times 1 \times 0.8 = 0.8 pu. Shaft output =0.8−0.15=0.65= 0.8 - 0.15 = 0.65 pu =32.5= 32.5 MW.

c) Field current reduced to zero

With Ef=0E_f = 0 only reluctance power remains:

Prel,max=V22(1Xq−1Xd)=12(2.5−1.25)=0.625 pu (at δ=45∘)P_{rel,max} = \frac{V^2}{2}\left(\frac{1}{X_q} - \frac{1}{X_d}\right) = \frac12(2.5 - 1.25) = 0.625\ \text{pu} \ (\text{at } \delta = 45^\circ)

The motor must take 0.80.8 pu (0.65 pu load + 0.15 pu rotational loss). Since 0.625<0.80.625 < 0.8, the reluctance torque cannot carry the load, so the machine falls out of synchronism. It would stay in step as a reluctance motor only if the shaft load were reduced so that total input is below 0.625 pu (load below 0.475 pu).

Answer: (a) Ef=0.728E_f = 0.728 pu (8.0 kV line), δ=22.8∘\delta = 22.8^\circ; (b) excitation power 0.353 pu (17.65 MW), saliency power 0.447 pu (22.35 MW); (c) No, it loses synchronism.

✓ Answer checked by Claude Sonnet 5.5

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