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N-R one iteration, P2 = 0.4 pu

Short answer

Jacobian matrix: J = [63, −21, 0; −21, 41, 0; 0, 0, 39]. Flat-start mismatches: ΔP2=0.4, ΔP3=−5, ΔQ3=−3. After one iteration: V2 = 1.05∠−2.37° pu, V3 = 0.9231∠−8.20° pu.

Figure below shows the single line diagram of 3 bus power system network. Determine the jacobian matrix, and perform load flow by N-R method up to one iteration. [Figure: bus 1 slack bus 1∠0° pu; bus 2 generator bus |V2| = 1.05 pu with P2 = 0.4 pu; bus 3 load bus (5 + j4) pu; line admittances y12 = −j40 pu, y13 = −j20 pu, y23 = −j20 pu]

Bus 1 is the slack bus (1∠0∘1\angle 0^\circ), bus 2 a generator (PV) bus (P2=0.4P_2 = 0.4 pu, ∣V2∣=1.05|V_2| = 1.05 pu) and bus 3 a load bus (P3=−5P_3 = -5 pu, Q3=−4Q_3 = -4 pu). Flat start: V20=1.05∠0∘V_2^0 = 1.05\angle 0^\circ, V30=1∠0∘V_3^0 = 1\angle 0^\circ. No Q-limits are given.

Y-bus

With y12=−j40y_{12} = -j40, y13=−j20y_{13} = -j20, y23=−j20y_{23} = -j20 pu:

Y11=y12+y13=−j60,Y22=y12+y23=−j60,Y33=y13+y23=−j40Y12=−y12=j40,Y13=−y13=j20,Y23=−y23=j20\begin{aligned} Y_{11} &= y_{12} + y_{13} = -j60, \quad Y_{22} = y_{12} + y_{23} = -j60, \quad Y_{33} = y_{13} + y_{23} = -j40 \\ Y_{12} &= -y_{12} = j40, \quad Y_{13} = -y_{13} = j20, \quad Y_{23} = -y_{23} = j20 \end{aligned} Ybus=[−j60.0000j40.0000j20.0000j40.0000−j60.0000j20.0000j20.0000j20.0000−j40.0000] puY_{bus} = \begin{bmatrix} -j60.0000 & j40.0000 & j20.0000 \\ j40.0000 & -j60.0000 & j20.0000 \\ j20.0000 & j20.0000 & -j40.0000 \end{bmatrix}\ \text{pu}

Calculated powers and mismatches

With Yij=∣Yij∣∠θijY_{ij} = |Y_{ij}|\angle\theta_{ij}, Vi=∣Vi∣∠δiV_i = |V_i|\angle\delta_i and ϕij=θij−δi+δj\phi_{ij} = \theta_{ij} - \delta_i + \delta_j:

Pi=∑j=1n∣Vi∣∣Vj∣∣Yij∣cos⁡ϕijQi=−∑j=1n∣Vi∣∣Vj∣∣Yij∣sin⁡ϕij\begin{aligned} P_i &= \sum_{j=1}^{n} |V_i||V_j||Y_{ij}|\cos\phi_{ij} \\ Q_i &= -\sum_{j=1}^{n} |V_i||V_j||Y_{ij}|\sin\phi_{ij} \end{aligned}

Jacobian elements (polar form, j≠ij \ne i):

∂Pi∂δi=∑j≠i∣Vi∣∣Vj∣∣Yij∣sin⁡ϕij∂Pi∂δj=−∣Vi∣∣Vj∣∣Yij∣sin⁡ϕij∂Pi∂∣Vi∣=2∣Vi∣∣Yii∣cos⁡θii+∑j≠i∣Vj∣∣Yij∣cos⁡ϕij∂Pi∂∣Vj∣=∣Vi∣∣Yij∣cos⁡ϕij∂Qi∂δi=∑j≠i∣Vi∣∣Vj∣∣Yij∣cos⁡ϕij∂Qi∂δj=−∣Vi∣∣Vj∣∣Yij∣cos⁡ϕij∂Qi∂∣Vi∣=−2∣Vi∣∣Yii∣sin⁡θii−∑j≠i∣Vj∣∣Yij∣sin⁡ϕij∂Qi∂∣Vj∣=−∣Vi∣∣Yij∣sin⁡ϕij\begin{aligned} \frac{\partial P_i}{\partial \delta_i} &= \sum_{j\ne i} |V_i||V_j||Y_{ij}|\sin\phi_{ij} \\ \frac{\partial P_i}{\partial \delta_j} &= -|V_i||V_j||Y_{ij}|\sin\phi_{ij} \\ \frac{\partial P_i}{\partial |V_i|} &= 2|V_i||Y_{ii}|\cos\theta_{ii} + \sum_{j\ne i} |V_j||Y_{ij}|\cos\phi_{ij} \\ \frac{\partial P_i}{\partial |V_j|} &= |V_i||Y_{ij}|\cos\phi_{ij} \\ \frac{\partial Q_i}{\partial \delta_i} &= \sum_{j\ne i} |V_i||V_j||Y_{ij}|\cos\phi_{ij} \\ \frac{\partial Q_i}{\partial \delta_j} &= -|V_i||V_j||Y_{ij}|\cos\phi_{ij} \\ \frac{\partial Q_i}{\partial |V_i|} &= -2|V_i||Y_{ii}|\sin\theta_{ii} - \sum_{j\ne i} |V_j||Y_{ij}|\sin\phi_{ij} \\ \frac{\partial Q_i}{\partial |V_j|} &= -|V_i||Y_{ij}|\sin\phi_{ij} \end{aligned}

At the flat start all cos⁡\cos terms are zero (θ=±90∘\theta = \pm 90^\circ, angles zero), so P20=P30=0P_2^0 = P_3^0 = 0:

P20=0.0000,Q20=3.1500P30=0.0000,Q30=−1.0000\begin{aligned} P_2^{0} &= 0.0000, \quad Q_2^{0} = 3.1500 \\ P_3^{0} &= 0.0000, \quad Q_3^{0} = -1.0000 \end{aligned} ΔP2=0.4000−(0.0000)=0.4000ΔP3=−5.0000−(0.0000)=−5.0000ΔQ3=−4.0000−(−1.0000)=−3.0000\begin{aligned} \Delta P_2 &= 0.4000 - (0.0000) = 0.4000 \\ \Delta P_3 &= -5.0000 - (0.0000) = -5.0000 \\ \Delta Q_3 &= -4.0000 - (-1.0000) = -3.0000 \end{aligned}

Jacobian matrix

∂P2∂δ2=(1.0500)(1.0000)(40.0000)sin⁡(90.00∘)+(1.0500)(1.0000)(20.0000)sin⁡(90.00∘)=63.0000∂P2∂δ3=−(1.0500)(1.0000)(20.0000)sin⁡(90.00∘)=−21.0000∂P2∂∣V3∣=(1.0500)(20.0000)cos⁡(90.00∘)=0.0000∂P3∂δ2=−(1.0000)(1.0500)(20.0000)sin⁡(90.00∘)=−21.0000∂P3∂δ3=(1.0000)(1.0000)(20.0000)sin⁡(90.00∘)+(1.0000)(1.0500)(20.0000)sin⁡(90.00∘)=41.0000∂P3∂∣V3∣=2(1.0000)(40.0000)cos⁡(−90.00∘)+(1.0000)(20.0000)cos⁡(90.00∘)+(1.0500)(20.0000)cos⁡(90.00∘)=0.0000∂Q3∂δ2=−(1.0000)(1.0500)(20.0000)cos⁡(90.00∘)=0.0000∂Q3∂δ3=(1.0000)(1.0000)(20.0000)cos⁡(90.00∘)+(1.0000)(1.0500)(20.0000)cos⁡(90.00∘)=0.0000∂Q3∂∣V3∣=−2(1.0000)(40.0000)sin⁡(−90.00∘)−(1.0000)(20.0000)sin⁡(90.00∘)−(1.0500)(20.0000)sin⁡(90.00∘)=39.0000\begin{aligned} \frac{\partial P_2}{\partial \delta_2} &= (1.0500)(1.0000)(40.0000)\sin(90.00^\circ) + (1.0500)(1.0000)(20.0000)\sin(90.00^\circ) = 63.0000 \\ \frac{\partial P_2}{\partial \delta_3} &= -(1.0500)(1.0000)(20.0000)\sin(90.00^\circ) = -21.0000 \\ \frac{\partial P_2}{\partial |V_3|} &= (1.0500)(20.0000)\cos(90.00^\circ) = 0.0000 \\ \frac{\partial P_3}{\partial \delta_2} &= -(1.0000)(1.0500)(20.0000)\sin(90.00^\circ) = -21.0000 \\ \frac{\partial P_3}{\partial \delta_3} &= (1.0000)(1.0000)(20.0000)\sin(90.00^\circ) + (1.0000)(1.0500)(20.0000)\sin(90.00^\circ) = 41.0000 \\ \frac{\partial P_3}{\partial |V_3|} &= 2(1.0000)(40.0000)\cos(-90.00^\circ) + (1.0000)(20.0000)\cos(90.00^\circ) + (1.0500)(20.0000)\cos(90.00^\circ) = 0.0000 \\ \frac{\partial Q_3}{\partial \delta_2} &= -(1.0000)(1.0500)(20.0000)\cos(90.00^\circ) = 0.0000 \\ \frac{\partial Q_3}{\partial \delta_3} &= (1.0000)(1.0000)(20.0000)\cos(90.00^\circ) + (1.0000)(1.0500)(20.0000)\cos(90.00^\circ) = 0.0000 \\ \frac{\partial Q_3}{\partial |V_3|} &= -2(1.0000)(40.0000)\sin(-90.00^\circ) - (1.0000)(20.0000)\sin(90.00^\circ) - (1.0500)(20.0000)\sin(90.00^\circ) = 39.0000 \end{aligned} [J0]=[63.0000−21.00000.0000−21.000041.00000.00000.00000.000039.0000][J^{0}] = \begin{bmatrix} 63.0000 & -21.0000 & 0.0000 \\ -21.0000 & 41.0000 & 0.0000 \\ 0.0000 & 0.0000 & 39.0000 \end{bmatrix}

First iteration

[0.4000−5.0000−3.0000]=[63.0000−21.00000.0000−21.000041.00000.00000.00000.000039.0000][Δδ2Δδ3Δ∣V3∣]\begin{bmatrix} 0.4000 \\ -5.0000 \\ -3.0000 \end{bmatrix} = \begin{bmatrix} 63.0000 & -21.0000 & 0.0000 \\ -21.0000 & 41.0000 & 0.0000 \\ 0.0000 & 0.0000 & 39.0000 \end{bmatrix}\begin{bmatrix} \Delta\delta_2 \\ \Delta\delta_3 \\ \Delta|V_3| \end{bmatrix} [Δδ2Δδ3Δ∣V3∣]=[J0]−1[0.4000−5.0000−3.0000]=[−0.0414−0.1431−0.0769]\begin{bmatrix} \Delta\delta_2 \\ \Delta\delta_3 \\ \Delta|V_3| \end{bmatrix} = [J^{0}]^{-1}\begin{bmatrix} 0.4000 \\ -5.0000 \\ -3.0000 \end{bmatrix} = \begin{bmatrix} -0.0414 \\ -0.1431 \\ -0.0769 \end{bmatrix} δ21=0+(−0.0414)=−0.0414 rad=−2.370∘δ31=0+(−0.1431)=−0.1431 rad=−8.201∘∣V3∣1=1.0000+(−0.0769)=0.9231 pu\begin{aligned} \delta_2^{1} &= 0 + (-0.0414) = -0.0414\ \text{rad} = -2.370^\circ \\ \delta_3^{1} &= 0 + (-0.1431) = -0.1431\ \text{rad} = -8.201^\circ \\ |V_3|^{1} &= 1.0000 + (-0.0769) = 0.9231\ \text{pu} \end{aligned}

So V21=1.0500∠−2.370∘V_2^{1} = 1.0500\angle -2.370^\circ pu and V31=0.9231∠−8.201∘V_3^{1} = 0.9231\angle -8.201^\circ pu.

Reactive power at bus 2 and slack bus power (with the new voltages):

Q21=−Im{V2∗∑kY2kVk}=4.9016 puQG2=Q2+QL2=4.9016 pu\begin{aligned} Q_2^{1} &= -\text{Im}\{V_2^{*}\textstyle\sum_k Y_{2k}V_k\} = 4.9016\ \text{pu} \\ Q_{G2} &= Q_2 + Q_{L2} = 4.9016\ \text{pu} \end{aligned} P1−jQ1=V1∗∑kY1kVk=(1.0000)(4.3703+j0.2368)=4.3703+j0.2368⇒P1=4.3703 pu,Q1=−0.2368 puPG1=P1+PL1=4.3703+0.00=4.3703 puQG1=Q1+QL1=−0.2368+0.00=−0.2368 pu\begin{aligned} P_1 - jQ_1 &= V_1^{*}\textstyle\sum_k Y_{1k}V_k = (1.0000)(4.3703 + j0.2368) \\ &= 4.3703 + j0.2368 \\ \Rightarrow P_1 &= 4.3703\ \text{pu},\quad Q_1 = -0.2368\ \text{pu} \\ P_{G1} &= P_1 + P_{L1} = 4.3703 + 0.00 = 4.3703\ \text{pu} \\ Q_{G1} &= Q_1 + Q_{L1} = -0.2368 + 0.00 = -0.2368\ \text{pu} \end{aligned}

Answer: J0=[63−210−214100039]J^0 = \begin{bmatrix} 63 & -21 & 0 \\ -21 & 41 & 0 \\ 0 & 0 & 39 \end{bmatrix}; after one iteration δ2=−2.370∘\delta_2 = -2.370^\circ, V3=0.9231∠−8.201∘V_3 = 0.9231\angle -8.201^\circ pu, QG2=4.9016Q_{G2} = 4.9016 pu, P1=4.3703P_1 = 4.3703 pu, Q1=−0.2368Q_1 = -0.2368 pu.

✓ Answer checked by Claude Sonnet 5.5

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