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Fault cleared at 45°: stability and maximum swing

Short answer

Initial power is 0.821 pu. During the three-phase fault at bus 1, electrical power is zero; clearing at 45° leaves the decelerating area larger than the accelerating area, so the system is stable and the maximum rotor swing is about 63.4°.

The power system shown below is operating initially at power angle δ = 20°. Calculate the power delivered to the infinite bus at normal operation. If a 3-phase to ground fault occurs at bus (1) and fault is cleared when the power angle δ reaches 45°, determine whether system come back to stable or not? If yes, calculate the maximum δ-swing angle. [Figure: generator E = 1.2 pu∠δ, j0.25 pu to bus (1); two parallel lines each j0.5 pu (breakers at both ends) from bus (1) to bus (2), the infinite bus V = 1 pu∠0°]

Data: E=1.2E = 1.2 pu, V=1V = 1 pu, Xd′=0.25X_d' = 0.25, two lines of 0.50.5 pu each, δ0=20∘\delta_0 = 20^\circ.

Assumption: the bus fault is temporary, so after clearing both lines are in service and the post-fault curve equals the pre-fault curve.

Step 1: Normal operation

X=0.25+0.52=0.5 pu,Pmax=1.2×10.5=2.4 puPe=2.4sin⁡20∘=0.8208 pu=Pm\begin{aligned} X &= 0.25 + \frac{0.5}{2} = 0.5\ \text{pu}, \qquad P_{max} = \frac{1.2\times1}{0.5} = 2.4\ \text{pu} \\ P_e &= 2.4\sin20^\circ = 0.8208\ \text{pu} = P_m \end{aligned}

Power delivered at normal operation: 0.821 pu.

Step 2: During the fault

A 3-phase fault at bus (1) puts the line-side voltage at zero, so Pe=0P_e = 0. The rotor accelerates from 20∘20^\circ to 45∘45^\circ.

A1=Pm(δc−δ0)=0.8208×(0.7854−0.3491)=0.3582 pu⋅radA_1 = P_m(\delta_c - \delta_0) = 0.8208\times(0.7854 - 0.3491) = 0.3582\ \text{pu·rad}

Step 3: Area available after clearing

δmax=180∘−20∘=160∘=2.7925 rad\delta_{max} = 180^\circ - 20^\circ = 160^\circ = 2.7925\ \text{rad} A2,max=Pmax(cos⁡45∘−cos⁡160∘)−Pm(δmax−δc)=2.4(0.7071+0.9397)−0.8208(2.7925−0.7854)=2.3048 pu⋅rad\begin{aligned} A_{2,max} &= P_{max}(\cos45^\circ - \cos160^\circ) - P_m(\delta_{max}-\delta_c) \\ &= 2.4(0.7071 + 0.9397) - 0.8208(2.7925 - 0.7854) \\ &= 2.3048\ \text{pu·rad} \end{aligned}

Since A2,max=2.305>A1=0.358A_{2,max} = 2.305 > A_1 = 0.358, the system is stable.

Step 4: Maximum swing angle δ1\delta_1

Set A2=A1A_2 = A_1:

2.4(cos⁡45∘−cos⁡δ1)−0.8208(δ1−0.7854)=0.35822.4(\cos45^\circ - \cos\delta_1) - 0.8208(\delta_1 - 0.7854) = 0.3582

Solving by trial (or numerically): δ1=1.1060\delta_1 = 1.1060 rad.

Answer: Power delivered = 0.821 pu; the system is stable; maximum swing δmax≈63.4∘\delta_{max} \approx 63.4^\circ.

For reference, the critical clearing angle for this case is cos⁡−1[(π−2δ0)sin⁡δ0−cos⁡δ0]=95.97∘\cos^{-1}[(\pi-2\delta_0)\sin\delta_0 - \cos\delta_0] = 95.97^\circ, so clearing at 45∘45^\circ leaves a wide margin.

✓ Answer checked by Claude Sonnet 5.5

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