TCIPG Reading Group – Fall 2012 Karl Reinhard & Ahmed Fawaz TCIPG 1 Trustworthy Cyber Infrastructure for the Power Grid University of Illinois

TCIPG Reading Group – Fall 2012

Karl Reinhard & Ahmed Fawaz

TCIPG

1Trustworthy Cyber Infrastructure for the Power Grid •

www.tcipg.orgUniversity of Illinois • Dartmouth College • Cornell University • UC Davis •

Washington State University

TCIPG Reading Group

Today’s Plan:• Discuss Read and Work Ahead• PowerWorld Snap Shot• A Peek into the Underlying Power Flow Equations• Next Week’s Plan

14 Sep 12

TCIPG Reading Group September 2012 2

Introduction

We seek to analyze the power system performance under steady state conditions.

The analysis in normal steady-state operation is called a power-flow study (load-flow study) and it targets on determining the Voltages, Currents, and Real and Reactive Power Flows in a system under specified generation and load conditions.

At each bus, We make an assumption about either

• a Voltage at a bus or

• the Power being supplied to the bus

Then determine

• Bus voltage magnitude and phase angles

• Line currents, etc. that would result


Basics for power-flow studies.

The way ahead…. to find the power-flow solution via iteration:

1. Create a bus admittance matrix Ybus for the power system;

2. Make an initial estimate for the voltages at each bus in the system;

3. Iterate to find conditions that satisfy the system’s load flow equations.

• Update the voltage estimate for each bus (one at a time), based on the estimates for the voltages and power flows at every other bus and the values of the bus admittance matrix.

• Since the voltage at a given bus depends on the voltages at all of the other busses in the system (which are just estimates), the updated voltage will not be correct. However, it will usually be closer to the answer than the original guess.

4. Repeat this process to make the voltages at each bus approaching the correct answers to within a set tolerance level…


Basics for power-flow studies

The equations used to update the estimates differ for each of 3 bus types.

1. Load bus (PQ bus) – All buses not having a generator

• Real and reactive power (P and Q)are specified

• Bus voltage magnitude and phase angle (V and q) will be calculated

• Real and reactive powers supplied to a power system are defined to be positive

• Powers consumed from the system are defined to be negative.

2. Generator bus (PV bus) –

• Voltage and real power supplied are specified

• Bus phase angle (q) will be calculated during iteration

• Reactive power will be calculated after the case’s solution is found


Basics for power-flow studies.

3. Slack bus (swing bus) –

• Special generator bus serving as the reference bus for the power system.

• Voltage is fixed – both magnitude and phase (for instance, 10˚ pu).

• Real and reactive powers are uncontrolled – supplies whatever real or reactive power is necessary to make the power flows in the system balance.

Key Points:

• Voltage on a load bus (P-Q bus) changes as the load varies – P and Q are fixed, while V (magnitude and angle) vary with load conditions.

• Generators (@ P-V buses) work most efficiently when running at full load – P and V are fixed

• Slack bus generator varies P and Q that it supplies to balance Complex power – V and Angle reference are fixed.


Ybus for power-flow analysis

12 32 42 2I I I I

31 42 2

21 21 23 24 23 24

1 1 1 VV VV I

Z Z Z Z Z Z

I12

I32

I42I2

2 32 1 2 42

21 23 24

V VV V V VI

Z Z Z

1 21 2 21 3 23 4 24 2VY V Y V Y V Y I

The basic equation for power-flow analysis is derived from the nodal analysis equations for the power system:

VV I R IR


Power-flow analysis equations

busV I Z Y V I

11 12 13 14 1 1

21 22 23 24 2 2

31 32 33 34 3 3

41 42 43 44 4 4

Y Y Y Y V I

Y Y Y Y V I

Y Y Y Y V I

Y Y Y Y V I

The basic equation for power-flow analysis is derived from the nodal analysis equations for the power system:

For the four-bus power system shown above, (1) becomes

where Yij are the elements of the bus admittance matrix, Vi are the bus voltages, and Ii are the currents injected at each node.

21 1 22 2 23 3 24 4 2Y V Y V Y V Y V I

(1)

(2)

(3)

For bus 2 in this system, this equation reduces to



1.7647 7.0588 0.5882 2.3529 0 1.1765 4.7059

0.5882 2.3529 1.5611 6.6290 0.3846 1.9231 0.5882 2.3529

0 0.3846 1.9231 1.5611 6.6290 1.1765 4.7059

1.1765 4.7059 0.5882 2.3529 1.1765 4.7059 2

bus

j j j

j j j jY

j j j

j j j

.9412 11.7647j

line #

Bus to bus

Series Z (pu)

Series Y (pu)

1 1-2 0.1+j0.4 0.5882-j2.3529

2 2-3 0.1+j0.5 0.3846-j1.9231

3 2-4 0.1+j0.4 0.5882-j2.3529

4 3-4 0.5+j0.2 1.1765-j4.7059

5 4-1 0.5+j0.2 1.1765-j4.7059

Example: a simple power system has 4 buses, 5 transmission lines, 1 generator, and 3 loads. Series per-unit impedances are:

Note: Ybus symmetric construction – Off diagonal elements are -Yij = -Yji



1.7647 7.0588 0.5882 2.3529 0 1.1765 4.7059

0.5882 2.3529 1.5611 6.6290 0.3846 1.9231 0.5882 2.3529

0 0.3846 1.9231 1.5611 6.6290 1.1765 4.7059

1.1765 4.7059 0.5882 2.3529 1.1765 4.7059 2

bus

j j j

j j j jY

j j j

j j j

.9412 11.7647j

line #

Bus to bus

Series Z (pu)

Series Y (pu)

1 1-2 0.1+j0.4 0.5882-j2.3529

2 2-3 0.1+j0.5 0.3846-j1.9231

3 2-4 0.1+j0.4 0.5882-j2.3529

4 3-4 0.5+j0.2 1.1765-j4.7059

5 4-1 0.5+j0.2 1.1765-j4.7059

Example: a simple power system has 4 buses, 5 transmission lines, 1 generator, and 3 loads. Series per-unit impedances are:

Note: Ybus symmetric construction – On diagonal elements:i j

ii ijY Y



However, real loads are specified in terms of real and reactive powers, not as currents. The relationship between per-unit real and reactive power supplied to the system at a bus and the per-unit current injected into the system at that bus is:

*S VI P jQ where V is the per-unit voltage at the bus; I* - complex conjugate of the per-unit current injected at the bus; P and Q are per-unit real and reactive powers. Therefore, for instance, the current injected at bus 2 can be found as

*

2 2* * 2 22 2 2 2 2 2 *

2 2

P jQP jQV I P jQ I I

V V

(4)

(5)

Substituting (5) into (3), we obtain

*

2 2

21 1 22 2 23 3 24 4 *2

P jQY V Y V Y V Y V

V

(6) ** * * *21 1 2 22 2 2 23 3 2 24 4 2 2 2Y VV Y V V Y VV Y V V P jQ



(6)

** * * * *2 2 2 21 1 2 22 2 2 23 3 2 24 4 2S P jQ Y VV Y V V Y VV Y V V

* *

1 1

( )ikn n

ji i i i ik k i k ik ik

k k

S P jQ V Y V V V e G jB

1

(cos sin )( )n

i k ik ik ik ikk

V V j G jB

1

1

Resolving into the real and imaginary parts:

( cos sin )

( sin cos )

n

i i k ik ik ik ik Gi Dik

n


P V V G B P P

Q V V G B Q Q



(6)

1

1

( cos sin )

( sin cos )

n


n


P V V G B P P

Q V V G B Q Q

2 2 2 2

n

2 2 2 2

( )

( )( )

( )

( )

G D

n Gn Dn

G D

n n Gn Dn

P P P

P P P

V Q Q Q

V Q Q Q

x

xx f x

x

x

G

BY


Non-Linear – Newton Raphson Soln

2

n

2

n

V

V

x

2 2 2

2 2 2

( )

( )( )

( )

( )

G D

n Gn Dn

G D

n Gn Dn

P P P

P P P

Q Q Q

Q Q Q

x

xf x

x

x


Information from power-flow studies

The basic information contained in the load-flow output is:

• All bus voltage magnitudes and phase angles w.r.t the slack bus.

• All bus active and reactive power injections.

• All line sending- and receiving-end complex power flows.

• Individual line losses can be deduced by subtracting receiving-end complex Power from sending-end complex power.

• Total system losses – deduced by summing complex power at all loads and generators and subtracting the totals.


Information from power-flow studies

The most important information obtained from the load-flow is the system voltage profile.

A power-flow program can be set up to provide alerts if the voltage at any given bus exceeds, for instance, 5% of the nominal value

such voltage variations may indicate problems…

• If │V│ varies greatly over the system, large reactive flows will result; this, in turn, will lead to increased real power losses and, in extreme cases, an increased likelihood of voltage collapse.

• When a particular bus has an unacceptably low voltage, the usual practice is to install capacitor banks in order to provide reactive compensation to the load.

Documents

TCIPG Reading Group – Fall 2012 Karl Reinhard & Ahmed Fawaz TCIPG 1 Trustworthy Cyber Infrastructure for the Power Grid University of Illinois