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22-Elec-B7 Power Systems Engineering · December 2013

Question 4 of 7: Bus Classification and a Three-Bus Power-Flow Calculation

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, December 2013 — 07-Elec-B7 Power Systems Engineering. Open-book, three hours, any non-communicating calculator permitted. Seven problems of equal value (20 points each); any five constitute a complete paper and only the first five appearing in the answer book are marked. All seven are solved here, because the set is a study resource.

Reference texts.

Problem 4: Bus Classification and a Three-Bus Power-Flow Calculation (20 points)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Part (a) — the three bus types of a conventional power flow. Each bus carries four quantities — $|V|$, $\delta$, $P$ and $Q$ — of which exactly two are specified and two are solved for.

In this problem bus 1 is the slack bus ($V_1=1.0\angle0^\circ$), bus 3 is a voltage-controlled bus whose magnitude and angle are both stated ($1.05\angle32^\circ$), and bus 2 is the load bus with $P_2=-4$ pu. The question removes the need to iterate by stipulating the bus-2 angle, which turns a Newton–Raphson solution into a set of direct substitutions.

Given. A three-bus system with two purely reactive tie lines, a slack machine at bus 1, a scheduled generator at bus 3, and a 4 pu real load at bus 2 whose angle is stipulated.

Given data
QuantitySymbolValue
Slack-bus voltage$V_1$$1.00\angle0^\circ$ pu
Bus-3 voltage$V_3$$1.05\angle32^\circ$ pu
Bus-2 real injection$P_2$$-4.0$ pu (load)
Bus-2 angle (stipulated)$\delta_2$$-7^\circ$
Line 1–2 reactance$X_{12}$$j0.08$ pu
Line 2–3 reactance$X_{23}$$j0.20$ pu

Find. $|V_2|$ and $Q_2$; then the real and reactive power generated at bus 1 and at bus 3.

[Figure not reproduced: Figure (2) redrawn. Both ties are purely reactive, so the network is lossless and the two generated real powers must sum to the 4 pu load exactly — a free check on the answer. See the official exam paper.]

Approach. Because both branches are purely reactive the general power-flow equations reduce to their lossless form; with $\delta_2$ stipulated, the bus-2 real-power equation is linear in $|V_2|$, and every remaining quantity is then a direct substitution.

  1. Write the lossless injection equations. For a network whose branches are pure reactances, the real and reactive power injected at bus $k$ towards bus $m$ are $$P_{km}=\frac{|V_k||V_m|}{X_{km}}\sin(\delta_k-\delta_m),\ Q_{km}=\frac{|V_k|^{2}}{X_{km}}-\frac{|V_k||V_m|}{X_{km}}\cos(\delta_k-\delta_m).$$ The bus injection is the sum over all lines leaving that bus.
  2. Part (b) — solve the bus-2 real-power equation for the voltage magnitude. Bus 2 is connected to buses 1 and 3, and the injection there is $-4$ pu. Both terms are proportional to $|V_2|$, so it factors out: $$-4=|V_2|\left[\frac{1.00}{0.08}\sin(-7^\circ)+\frac{1.05}{0.20}\sin(-7^\circ-32^\circ)\right],$$ $$-4=|V_2|\left[12.5(-0.121869)+5.25(-0.629320)\right]=|V_2|(-1.52336-3.30393),$$ $$\boxed{|V_2|=\frac{-4}{-4.82729}=0.8286\ \text{pu}}$$
  3. Substitute back for the reactive injection at bus 2. With $|V_2|$ now known, $$Q_2=|V_2|^{2}\left(\frac{1}{0.08}+\frac{1}{0.20}\right)-\frac{|V_2|(1.00)}{0.08}\cos(-7^\circ)-\frac{|V_2|(1.05)}{0.20}\cos(-39^\circ),$$ $$Q_2=0.686571(17.5)-10.28197-3.38087=12.01500-13.66284,$$ $$\boxed{Q_2=-1.6456\ \text{pu (the bus 2 load absorbs 1.646 pu)}}$$
  4. Part (c) — take the injection at the slack bus. Bus 1 has only the one tie, to bus 2, so $$P_1=\frac{|V_1||V_2|}{X_{12}}\sin(\delta_1-\delta_2)=12.5(0.828621)\sin(7^\circ),$$ $$Q_1=\frac{|V_1|^{2}}{X_{12}}-\frac{|V_1||V_2|}{X_{12}}\cos(7^\circ)=12.50000-10.28197,$$ $$\boxed{P_1=1.2623\ \text{pu},\ Q_1=2.2194\ \text{pu}}$$
  5. Part (d) — take the injection at bus 3. Bus 3 also has a single tie, to bus 2, and the angle across it is $32^\circ-(-7^\circ)=39^\circ$: $$P_3=\frac{(1.05)(0.828621)}{0.20}\sin39^\circ=4.35026(0.629320),$$ $$Q_3=\frac{(1.05)^{2}}{0.20}-4.35026\cos39^\circ=5.51250-3.38087,$$ $$\boxed{P_3=2.7377\ \text{pu},\ Q_3=2.1317\ \text{pu}}$$
  6. Check the balance the lossless network guarantees. With no series resistance anywhere, the generated real powers must equal the load exactly: $$P_1+P_3=1.26229+2.73771=4.00000\ \text{pu}=|P_2|.$$ The reactive powers do not balance, and should not: the series reactances absorb $Q_1+Q_3-|Q_2|=2.21945+2.13171-1.64562=2.70554$ pu, which is $\sum I^{2}X$ in the two lines.
  7. Read the result as an operating engineer would. The stipulated $-7^\circ$ angle at bus 2 forces the load-bus voltage down to 0.829 pu, roughly 12 % below the acceptable lower limit of about 0.95 pu. The diagnosis is visible in the numbers: bus 2 draws 4 pu of real power and 1.65 pu of reactive power through two reactances that consume 2.71 pu of vars between them, and there is no reactive source at the load bus at all. Shunt capacitors or a static var compensator at bus 2 — or scheduling bus 3 harder so more of the transfer arrives over the shorter tie — is what a planning study would recommend next.

Check: the question fixes $\delta_2=-7^\circ$ rather than letting it be solved, so this is not a converged Newton–Raphson solution of the whole network; it is the (perfectly well-posed) inverse problem of finding what $|V_2|$ and $Q_2$ must be given that angle. A conventional power flow, with $Q_2$ specified instead, would return a slightly different angle-magnitude pair.

QuantitySymbol Result
Bus-2 voltage magnitude$|V_2|$0.8286 pu
Bus-2 reactive injection$Q_2$−1.6456 pu
Bus-1 real generation$P_1$1.2623 pu
Bus-1 reactive generation$Q_1$2.2194 pu
Bus-3 real generation$P_3$2.7377 pu
Bus-3 reactive generation$Q_3$2.1317 pu
Real-power balance check$P_1+P_3$4.0000 pu