Newton-Raphson (polar form) is applied to the two-bus system; the line has z=0.12+j0.16 pu, and the load of 100 MW + j50 MVAr becomes 1+j0.5 pu on the 100 MVA base.
Bus data and Y-bus
Base 100 MVA. Bus 1: slack, V1=1∠0∘. Bus 2: load bus with P2=−1.00 pu and Q2=−0.50 pu (negative, as power is taken out). Unknowns: δ2, ∣V2∣. Flat start: ∣V2∣(0)=1, δ2(0)=0.
y12Y11Y12=0.12+j0.161=0.040.12−j0.16=3−j4=Y22=y12=3.0000−j4.0000=5.0000∠−53.13∘=Y21=−y12=−3.0000+j4.0000=5.0000∠126.87∘
Equations used
With Yij=∣Yij∣∠θij, Vi=∣Vi∣∠δi and ϕij=θij−δi+δj:
PiQi=j=1∑n∣Vi∣∣Vj∣∣Yij∣cosϕij=−j=1∑n∣Vi∣∣Vj∣∣Yij∣sinϕij
Jacobian elements (polar form, j=i):
∂δi∂Pi∂δj∂Pi∂∣Vi∣∂Pi∂∣Vj∣∂Pi∂δi∂Qi∂δj∂Qi∂∣Vi∣∂Qi∂∣Vj∣∂Qi=j=i∑∣Vi∣∣Vj∣∣Yij∣sinϕij=−∣Vi∣∣Vj∣∣Yij∣sinϕij=2∣Vi∣∣Yii∣cosθii+j=i∑∣Vj∣∣Yij∣cosϕij=∣Vi∣∣Yij∣cosϕij=j=i∑∣Vi∣∣Vj∣∣Yij∣cosϕij=−∣Vi∣∣Vj∣∣Yij∣cosϕij=−2∣Vi∣∣Yii∣sinθii−j=i∑∣Vj∣∣Yij∣sinϕij=−∣Vi∣∣Yij∣sinϕij
For bus 2, [ΔP2; ΔQ2]=J[Δδ2; Δ∣V2∣].
Newton-Raphson iterations
Iteration 1
Calculated powers and mismatches with the values from iteration 0:
P2(0)Q2(0)=0.0000,ΔP2=−1.0000−(0.0000)=−1.0000=0.0000,ΔQ2=−0.5000−(0.0000)=−0.5000
Jacobian elements:
∂δ2∂P2∂∣V2∣∂P2∂δ2∂Q2∂∣V2∣∂Q2=(1.0000)(1.0000)(5.0000)sin(126.87∘)=4.0000=2(1.0000)(5.0000)cos(−53.13∘)+(1.0000)(5.0000)cos(126.87∘)=3.0000=(1.0000)(1.0000)(5.0000)cos(126.87∘)=−3.0000=−2(1.0000)(5.0000)sin(−53.13∘)−(1.0000)(5.0000)sin(126.87∘)=4.0000
[−1.0000−0.5000]=[4.0000−3.00003.00004.0000][Δδ2Δ∣V2∣]
[Δδ2Δ∣V2∣]=[−0.1000−0.2000]
δ2(1)∣V2∣(1)=0.0000+(−0.1000)=−0.1000 rad=−5.7296∘=1.0000+(−0.2000)=0.8000 pu
Iteration 2
Calculated powers and mismatches with the values from iteration 1:
P2(1)Q2(1)=−0.7875,ΔP2=−1.0000−(−0.7875)=−0.2125=−0.3844,ΔQ2=−0.5000−(−0.3844)=−0.1156
Jacobian elements:
∂δ2∂P2∂∣V2∣∂P2∂δ2∂Q2∂∣V2∣∂Q2=(0.8000)(1.0000)(5.0000)sin(132.60∘)=2.9444=2(0.8000)(5.0000)cos(−53.13∘)+(1.0000)(5.0000)cos(132.60∘)=1.4157=(0.8000)(1.0000)(5.0000)cos(132.60∘)=−2.7075=−2(0.8000)(5.0000)sin(−53.13∘)−(1.0000)(5.0000)sin(132.60∘)=2.7195
[−0.2125−0.1156]=[2.9444−2.70751.41572.7195][Δδ2Δ∣V2∣]
[Δδ2Δ∣V2∣]=[−0.0350−0.0773]
δ2(2)∣V2∣(2)=−0.1000+(−0.0350)=−0.1350 rad=−7.7345∘=0.8000+(−0.0773)=0.7227 pu
i) Bus 2 voltage after the 2nd iteration
∣V2∣=0.7227 pu, δ2=−7.735∘, i.e. V2=0.7227∠−7.735∘ pu.
ii) Slack bus power and network losses
S1=P1+jQ1=V1[Y11V1+Y12V2]∗=1.2408+j0.8439 pu=124.08 MW+j84.39 MVAr
I12SlossPloss=(V1−V2)y12=1.2408−j0.8439=1.5006∠−34.2208∘ pu=S12+S21=V1I12∗−V2I12∗=0.2702+j0.3603 pu=27.02 MW,Qloss=36.03 MVAr
(The loss is found from the line current with the 2nd-iteration voltages. If it is instead taken as S1−Sload, it gives 0.2408+j0.3439 pu; the two differ because after two iterations the calculated bus 2 power has not yet reached the specified load (the solution is not fully converged). The converged answer is V2=0.7071∠−8.130∘ pu.)
Answer: V2=0.7227∠−7.735∘ pu; slack bus supplies P1=124.08 MW and Q1=84.39 MVAr; losses ≈27.02 MW and 36.03 MVAr.