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.
M. E. El-Hawary, Electrical Power Systems: Design and Analysis,
rev. ed., IEEE Press/Wiley — the notation this paper uses throughout
(the ABCD two-port, the salient-pole power-angle expressions, the sequence
networks and the equal-area criterion).
J. D. Glover, T. J. Overbye and M. S. Sarma, Power System Analysis and
Design, 6th ed., Cengage — transmission-line parameters and the exact
long line (Ch. 4–5), power flow (Ch. 6), symmetrical faults (Ch. 7),
symmetrical components and unsymmetrical faults (Ch. 8–9), transient
stability (Ch. 11).
J. J. Grainger and W. D. Stevenson, Power System Analysis,
McGraw-Hill — three-winding transformers, sequence networks and the
bus-impedance method.
S. J. Chapman, Electric Machinery Fundamentals, 5th ed.,
McGraw-Hill — transformers (Ch. 2) and synchronous machines
(Ch. 4–5).
Canadian practice: CSA C22.3 No. 1 Overhead Systems, CAN/CSA-C88
and CSA C50 (power transformers and insulating oil), and IEEE C37.91 as adopted
by Canadian utilities for transformer protection.
Problem 4: Bus Classification and a Three-Bus Power-Flow Calculation (20 points)
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.
Slack (swing, reference) bus.Known: $|V|$ and
$\delta$ (the angle is fixed at zero to define the reference).
Unknown: $P$ and $Q$. There is one such bus per island. It exists
because the network losses are not known until the solution is complete, so one
generator must be left free to make up whatever real and reactive power the
balance demands.
Voltage-controlled (PV, generator) bus.Known: $P$
(set by the turbine governor) and $|V|$ (held by the automatic voltage
regulator). Unknown: $Q$ and $\delta$. If the solved $Q$ violates the
machine's var limit, the bus is reclassified as a PQ bus at the violated limit
and the solution is repeated.
Load (PQ) bus.Known: $P$ and $Q$, both taken from
the load forecast (negative injections for load). Unknown: $|V|$ and
$\delta$. Most buses in a real study are of this type, including every bus with
no generation at all.
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
Quantity
Symbol
Value
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.
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.
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:
$$-4=|V_2|\left[\frac{1.00}{0.08}\sin(-7^\circ)+\frac{1.05}{0.20}\sin(-7^\circ-32^\circ)\right],$$
$$-4=|V_2|\left[12.5(-0.121869)+5.25(-0.629320)\right]=|V_2|(-1.52336-3.30393),$$
$$\boxed{|V_2|=\frac{-4}{-4.82729}=0.8286\ \text{pu}}$$
Substitute back for the reactive injection at bus 2.
With $|V_2|$ now known,
$$Q_2=|V_2|^{2}\left(\frac{1}{0.08}+\frac{1}{0.20}\right)-\frac{|V_2|(1.00)}{0.08}\cos(-7^\circ)-\frac{|V_2|(1.05)}{0.20}\cos(-39^\circ),$$
$$Q_2=0.686571(17.5)-10.28197-3.38087=12.01500-13.66284,$$
$$\boxed{Q_2=-1.6456\ \text{pu (the bus 2 load absorbs 1.646 pu)}}$$
Part (c) — take the injection at the slack bus.
Bus 1 has only the one tie, to bus 2, so
$$P_1=\frac{|V_1||V_2|}{X_{12}}\sin(\delta_1-\delta_2)=12.5(0.828621)\sin(7^\circ),$$
$$Q_1=\frac{|V_1|^{2}}{X_{12}}-\frac{|V_1||V_2|}{X_{12}}\cos(7^\circ)=12.50000-10.28197,$$
$$\boxed{P_1=1.2623\ \text{pu},\ Q_1=2.2194\ \text{pu}}$$
Part (d) — take the injection at bus 3. Bus 3 also
has a single tie, to bus 2, and the angle across it is
$32^\circ-(-7^\circ)=39^\circ$:
$$P_3=\frac{(1.05)(0.828621)}{0.20}\sin39^\circ=4.35026(0.629320),$$
$$Q_3=\frac{(1.05)^{2}}{0.20}-4.35026\cos39^\circ=5.51250-3.38087,$$
$$\boxed{P_3=2.7377\ \text{pu},\ Q_3=2.1317\ \text{pu}}$$
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.
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.