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Lecture 14 Power Flows Read: Chapter 6.1 – 6.6, 6.8 –6.11 Midterm Exam is on March 8 st Dr. Lei Wu Department of Electrical and Computer Engineering EE 333 POWER SYSTEMS ENGINEERING
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Page 1: Lecture EE333 - lecture 14

Lecture 14

Power Flows

Read: Chapter 6.1 – 6.6, 6.8 –6.11

Midterm Exam is on March 8st

Dr. Lei Wu

Department of Electrical and Computer Engineering

EE 333

POWER SYSTEMS ENGINEERING

Page 2: Lecture EE333 - lecture 14

2

IEEE Power and Energy Society—

Interest meeting--

Formation of a Clarkson Student Chapter

Wednesday March 7

5pm

CAMP 178

IEEE Power and Energy Society (PES) is the primary professional group for power engineers. Being a

member of a PES student chapter is an indication of your interest in power engineering. Members have

access to PES publications, particularly the Power and Energy Magazine, which reports on state of the art

issues in power engineering. A power engineering student chapter at Clarkson will allow us to hold power

engineering oriented meetings and projects, potential activities will be discussed at the meeting.

Page 3: Lecture EE333 - lecture 14

Outline

� Bus-branch model of power systems

� The power flow problem

� Iterative methods for solving nonlinear equations

� Approximations to the power flow problem

3

Page 4: Lecture EE333 - lecture 14

Bus-Branch Model of Power Systems

� A power system includes

� Loads

� Generators

� Transmission lines

� Transformers

4

Page 5: Lecture EE333 - lecture 14

Load Models

� Ultimate goal is to supply loads with electricity at constant

frequency and voltage

� Electrical characteristics of individual loads matter, but usually

they can only be estimated actual loads are constantly changing,

consisting of a large number of individual devices only limited

network observability of load characteristics

� Aggregate models are typically used for analysis

� Two common models

� constant power: Si = Pi + jQi

� constant impedance: Si = |V|2 / Zi

5

Page 6: Lecture EE333 - lecture 14

Generator Models

� Engineering models depend upon application

� Generators are usually synchronous machines

� For generators we will use two different models:

� a steady-state model, treating the generator as a constant power

source operating at a fixed voltage; this model will be used for

power flow and economic analysis

� a short term model treating the generator as a constant voltage

source behind a possibly time-varying reactance

6

Page 7: Lecture EE333 - lecture 14

Bus-branch model of power systems

� A power system includes

� Transmission lines

� Transformers

7

� Generators

� Loads

Page 8: Lecture EE333 - lecture 14

Power Flow Problem

� The most common power system analysis tool is the power flow

(also known sometimes as the load flow)

� Power flow determines how the power flows in a network under balanced

three-phase steady-state conditions.

� Also determines all bus voltages and all currents, as well as equipment

losses can be obtained

� Because of constant power models, power flow is a nonlinear problem

� Power flow is a steady-state analysis tool

� Each bus has 4 variables:

� P

� Q

� V

� δ

8

Page 9: Lecture EE333 - lecture 14

� Bus types

� Reference bus (VΘ bus) : Usually select a bus with a large

generator, , calculate P and Q.

� PQ bus: load buses where P and Q are given, calculate V and δ

� PV bus: Voltage controlled buses ( typically are buses with

generators) where P and V are given, calculate Q and δ.

� Usually Q of a generator is limited by Qmin and Qmax, which are

dependent upon the generator's MW output

� In the calculation procedure

� if Q < Qmin, fix Q = Qmin

� If Q > Qmax, fix Q = Qmax

� "type-switching“: Change the bus type to PQ and continue the

calculation procedure.

9

1 0o∠

Page 10: Lecture EE333 - lecture 14

� Bus types

� Reference bus (VΘ bus) : Usually select a bus with a large

generator, , calculate P and Q.

� PQ bus: load buses where P and Q are given, calculate V and δ

� PV bus: Voltage controlled buses ( typically are buses with

generators) where P and V are given, calculate Q and δ.

10

1 0o∠

Page 11: Lecture EE333 - lecture 14

Linear VS Nonlinear systems

� f(x) is a linear system as long as

� f(ax+by) = a*f(x) + b*f(y)

� The output is proportional to the input

� The principle of superposition holds

� Linear example f(x) = c*x

� Nonlinear example f(x) = cx2 , f(x) = c*sin(x)

11

Page 12: Lecture EE333 - lecture 14

Linear Power System Elements

� Linear circuit elements, which may be analyzed by

superposition.

� Resistor

� Inductor

� Capacitor

� Independent voltage and current sources

V = R I

V =

1V =

j L I

Ij C

ω

ω

Page 13: Lecture EE333 - lecture 14

Nonlinear Power System Elements

� Constant power loads and generator injections are nonlinear

and hence systems with these elements can not be analyzed by

superposition

� Nonlinear problems can be very difficult to solve, and usually

require an iterative approach

� Gauss-Seidel (G-S)

� Newton-Raphson (N-R)

13

Page 14: Lecture EE333 - lecture 14

Nonlinear Systems May Have Multiple Solutions or No Solution

� Example 1: x2 - 2 = 0 has real solutions x = ± 2

� Example 2: x2 + 2 = 0 has no real solution

14

f(x) = x2 - 2 f(x) = x2 + 2

two solutions where f(x) = 0 no solution f(x) = 0

Page 15: Lecture EE333 - lecture 14

Gauss Iteration

� With the Gauss method, we need to rewrite the equation in an

implicit form x= h(x).

� To iterate, we first make an initial guess of x, x(0) , and then

iteratively solve x(k+1)= h(x(k)), until we find a fixed point, x, such

that x= h(x).

� Stopping criterion

15

( ) ( ) ( 1) ( )

( ) 22

1

i

If x is a scalar with

If x is a vector with

OR max x

v v v v

nv

iji

i

x x x x

x x

ε

ε

+

=

∆ < ∆ −

∆ < ∆ = ∆

∆ = ∆

∑x

x

Page 16: Lecture EE333 - lecture 14

Gauss Iteration Example

( 1) ( )

(0)

( ) ( )

Example: Solve - 1 0

1

Let = 0 and arbitrarily guess x 1 and solve

0 1 5 2.61185

1 2 6 2.61612

2 2.41421 7 2.61744

3 2.55538 8 2.61785

4 2.59805 9 2.61798

v v

v v

x x

x x

v

v x v x

+

− =

= +

=

Page 17: Lecture EE333 - lecture 14

Power Flow Analysis - Gauss

� We know neither complex bus voltages nor complex current injections

� Rather, we know the complex power being consumed by the load, and

the power being injected by generators plus their voltage magnitudes

17

bus=I Y V1

N

k kn nn

Y V=

= ∑I

* * *

1

N

k k k k k k kn nn

S P jQ V I V Y V=

= + = = ∑* * *

1

N

k k k k k k kn nn

S P jQ V I V Y V=

= − = = ∑* 1

*1 1 1

N k Nk

kn n kk k kn n kn nn n n kk

SY V Y V Y V Y V

V

= = = += = + +∑ ∑ ∑

* 1

*1 1

1 k Nk

k kn n kn nkk n n kk

SV Y V Y V

Y V

= = +

= − −

∑ ∑

Page 18: Lecture EE333 - lecture 14

Three-Bus Power Flow Example –Gauss-Seidel

18

20 50 10 20 10 30

10 20 26 52 16 32

10 30 16 32 26 62bus

j j j

Y j j j

j j j

− − + − + = − + − − + − + − + −

V Θ P Q

Bus 1 1.05 0 ? ?

Bus 2 ? (1) ? (0) -4 -2.5

Bus 3 1.04 ? (0) +2 ?

Using the MVA base of 100MVA


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