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Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

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Page 1: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

Lecture 22 Unbalanced Faults and Power System Protection

Professor Tom OverbyeDepartment of Electrical and

Computer Engineering

ECE 476

POWER SYSTEM ANALYSIS

Page 2: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

2

Announcements

Design Project 2 from the book (page 345 to 348) was due on Nov 15, but I have given you an extension to Nov 29. The Nov 29 date is firm!

Be reading Chapters 8 and 9 HW 10 is 8.3, 8.4, 9.1,9.2 (bus 2), 9.13, 9.51 is due on

Thursday Final is Wednesday Dec 12 from 1:30 to 4:30pm in EL

269 (note room change). Final is comprehensive. One new note sheet, and your two old note sheets are allowed

Page 3: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

3

Double Line-to-Ground Faults

With a double line-to-ground (DLG) fault two line conductors come in contact both with each other and ground. We'll assume these are phases b and c.

0 ( )f f f f fa cg f cbg bI V V Z I I

Page 4: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

4

DLG Faults, cont'd

0

2

2

0

From the current relationships we get

1 1 1

1

1

Since 0 0

Note, because of the path to ground the zero

sequence current is no longer

ffa

ffb

fc f

fa f f f

II

I I

I I

I I I I

zero.

Page 5: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

5

DLG Faults, cont'd

0

2

2

0 2

2 2

0

From the voltage relationships we get

1 1 11

13

1

Since

Then ( )

But since 1 0 1

ff ag

ff bg

ff bg

f fcg f fbg

ff fbg

ff fbg

V V

V V

V V

V V V V

V V V

V V V

Page 6: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

6

DLG Faults, cont'd

0

0 2

0 2

2

0 0

0 0

( )

Also, since

Adding these together (with -1)

(2 ) with

3

ff fbg

f ff cb

ff f fb

fc f f f

ff f f f f f fbg

f f f f

V V V

Z I I

I I I I

I I I I

V Z I I I I I I

V V Z I

Page 7: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

7

DLG Faults, cont'd

The three sequence networks are joined as follows

0

1.05 00.1389 0.092( 3 )

4.547 0

ff

VI

j jZ Z Z Z

Assuming Zf=0, then

Page 8: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

8

DLG Faults, cont'd

0

1.05 4.547 90 0.1389 0.4184

0.4184/ 0.1456 2.874

4.547 2.874 1.673

Converting to phase: 1.04 6.82

1.04 6.82

f

f

f f f

fb

fc

V j

I j j

I I I j j j

I j

I j

Page 9: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

9

Unbalanced Fault Summary

SLG: Sequence networks are connected in series, parallel to three times the fault impedance

LL: Positive and negative sequence networks are connected in parallel; zero sequence network is not included since there is no path to ground

DLG: Positive, negative and zero sequence networks are connected in parallel, with the zero sequence network including three times the fault impedance

Page 10: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

10

Generalized System Solution

Assume we know the pre-fault voltages The general procedure is then

1. Calculate Zbus for each sequence

2. For a fault at bus i, the Zii values are the thevenin equivalent impedances; the pre-fault voltage is the positive sequence thevenin voltage

3. Connect and solve the thevenin equivalent sequence networks to determine the fault current

4. Sequence voltages throughout the system are

Page 11: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

11

Generalized System Solution, cont’d

4. Sequence voltages throughout the system are given by 0

0

0

0

prefaultfIZ

V V

This is solvedfor each sequence network!

5. Phase values are determined from the sequence values

Page 12: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

12

Unbalanced System Example

For the generators assume Z+ = Z = j0.2; Z0 = j0.05For the transformers assume Z+ = Z =Z0 = j0.05For the lines assume Z+ = Z = j0.1; Z0 = j0.3

Assume unloaded pre-fault, with voltages =1.0 p.u.

Page 13: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

13

Positive/Negative Sequence Network

24 10 10 0.1397 0.1103 0.125

10 24 10 0.1103 0.1397 0.125

10 10 20 0.1250 0.1250 0.175bus busj j

Y Z

Negative sequence is identical to positive sequence

Page 14: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

14

Zero Sequence Network

0 0

16.66 3.33 3.33 0.0732 0.0148 0.0440

3.33 26.66 3.33 0.0148 0.0435 0.0.292

3.33 3.33 6.66 0.0440 0.0292 0.1866bus busj j

Y Z

Page 15: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

15

For a SLG Fault at Bus 3

The sequence networks are created using the pre-faultvoltage for the positive sequence thevenin voltage,and the Zbus diagonals for the thevenin impedances

Positive Seq. Negative Seq. Zero Seq.

The fault type then determines how the networks areinterconnected

Page 16: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

16

Bus 3 SLG Fault, cont’d

0

1.0 01.863

(0.1750 0.1750 0.1866)

1.863

1.0 0 0 0.7671

1.0 0 0 0.7671

1.0 0 1.863 0.6740

0 0.2329

0 0.2329

1.863 0.3260

f

f f f

bus

bus

I jj

I I I j

j

j

V Z

V Z

Page 17: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

17

Bus 3 SLG Fault, cont’d

0 0

3

1

0 0.0820

0 0.0544

1.863 0.3479

We can then calculate the phase voltages at any bus

0.3479 0

0.6740 0.522 0.866

0.3260 0.522 0.866

0.0820

0.7671

bus

j

j

j

V Z

V A

V A

0.4522

0.3491 0.866

0.2329 0.3491 0.866

j

j

Page 18: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

18

Faults on Lines

The previous analysis has assumed that the fault is at a bus. Most faults occur on transmission lines, not at the buses

For analysis these faults are treated by including a dummy bus at the fault location. How the impedance of the transmission line is then split depends upon the fault location

Page 19: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

19

Line Fault Example

Assume a SLG fault occurs on the previous system on the line from bus 1 to bus 3, one third of the wayfrom bus 1 to bus 3. To solve the system we add adummy bus, bus 4, at the fault location

Page 20: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

20

Line Fault Example, cont’d

44 10 0 30

10 24 10 0

0 10 25 15

30 0 15 45

Adding the dummy bus only changes the new

row/column entries associated with the dummy bus

0.1397 0.1103 0.1250 0.1348

0.1103 0.1397 0.1250 0.1152

0.125

bus

bus

j

j

Y

Z0 0.1250 0.1750 0.1417

0.1348 0.1152 0.1417 0.1593

The Ybus

now has4 buses

Page 21: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

21

Power System Protection

Main idea is to remove faults as quickly as possible while leaving as much of the system intact as possible

Fault sequence of events1. Fault occurs somewhere on the system, changing the

system currents and voltages

2. Current transformers (CTs) and potential transformers (PTs) sensors detect the change in currents/voltages

3. Relays use sensor input to determine whether a fault has occurred

4. If fault occurs relays open circuit breakers to isolate fault

Page 22: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

22

Power System Protection

Protection systems must be designed with both primary protection and backup protection in case primary protection devices fail

In designing power system protection systems there are two main types of systems that need to be considered:

1. Radial: there is a single source of power, so power always flows in a single direction; this is the easiest from a protection point of view

2. Network: power can flow in either direction: protection is much more involved

Page 23: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

23

Radial Power System Protection

Radial systems are primarily used in the lower voltage distribution systems. Protection actions usually result in loss of customer load, but the outages are usually quite local.

The figure showspotential protectionschemes for a radial system. Thebottom scheme ispreferred since itresults in less lost load

Page 24: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

24

Radial Power System Protection

In radial power systems the amount of fault current is limited by the fault distance from the power source: faults further done the feeder have less fault current since the current is limited by feeder impedance

Radial power system protection systems usually use inverse-time overcurrent relays.

Coordination of relay current settings is needed toopen the correct breakers

Page 25: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

25

Inverse Time Overcurrent Relays

Inverse time overcurrent relays respond instan-taneously to a current above their maximum setting

They respond slower to currents below this value but above the pickup current value

Page 26: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

26

Inverse Time Relays, cont'd

The inverse time characteristic provides backup protection since relays further upstream (closer to power source) should eventually trip if relays closer to the fault fail

Challenge is to make sure the minimum pickup current is set low enough to pick up all likely faults, but high enough not to trip on load current

When outaged feeders are returned to service there can be a large in-rush current as all the motors try to simultaneously start; this in-rush current may re-trip the feeder

Page 27: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

27

Inverse Time Overcurrent Relays

Relays havetraditionally beenelectromechanicaldevices, but aregradually beingreplaced by digital relays

Current and timesettings are ad-justed using dialson the relay

Page 28: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

28

Protection of Network Systems

In a networked system there are a number of difference sources of power. Power flows are bidirectional

Networked system offer greater reliability, since the failure of a single device does not result in a loss of load

Networked systems are usually used with the transmission system, and are sometimes used with the distribution systems, particularly in urban areas

Page 29: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

29

Network System Protection

Removing networked elements require the opening of circuit breakers at both ends of the device

There are several common protection schemes; multiple overlapping schemes are usually used

1. Directional relays with communication between the device terminals

2. Impedance (distance) relays.

3. Differential protection

Page 30: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

30

Directional Relays

Directional relays are commonly used to protect high voltage transmission lines

Voltage and current measurements are used to determine direction of current flow (into or out of line)

Relays on both ends of line communicate and will only trip the line if excessive current is flowing into the line from both ends

– line carrier communication is popular in which a high frequency signal (30 kHz to 300 kHz) is used

– microwave communication is sometimes used

Page 31: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

31

Impedance Relays

Impedance (distance) relays measure ratio of voltage to current to determine if a fault exists on a particular line

1 1

12 12

Assume Z is the line impedance and x is the

normalized fault location (x 0 at bus 1, x 1 at bus 2)

V VNormally is high; during fault

I IxZ

Page 32: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

32

Impedance Relays Protection Zones

To avoid inadvertent tripping for faults on other transmission lines, impedance relays usually have several zones of protection:

– zone 1 may be 80% of line for a 3 fault; trip is instantaneous– zone 2 may cover 120% of line but with a delay to prevent

tripping for faults on adjacent lines– zone 3 went further; being removed due to 8/14/03 events

The key problem is that different fault types will present the relays with different apparent impedances; adequate protection for a 3 fault gives very limited protection for LL faults

Page 33: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

33

Impedance Relay Trip Characteristics

Source: August 14th 2003 Blackout Final Report, p. 78

Page 34: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

34

Differential Relays

Main idea behind differential protection is that during normal operation the net current into a device should sum to zero for each phase

– transformer turns ratios must, of course, be considered

Differential protection is used with geographically local devices

– buses– transformers– generators

1 2 3 0 for each phase

except during a fault

I I I

Page 35: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

35

Other Types of Relays

In addition to providing fault protection, relays are used to protect the system against operational problems as well

Being automatic devices, relays can respond much quicker than a human operator and therefore have an advantage when time is of the essence

Other common types of relays include– under-frequency for load: e.g., 10% of system load must be shed if

system frequency falls to 59.3 Hz– over-frequency on generators– under-voltage on loads (less common)

Page 36: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

36

Sequence of Events Recording

During major system disturbances numerous relays at a number of substations may operate

Event reconstruction requires time synchronization between substations to figure out the sequence of events

Most utilities now have sequence of events recording that provide time synchronization of at least 1 microsecond

Page 37: Lecture 22 Unbalanced Faults and Power System Protection Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS

37

Use of GPS for Fault Location

Since power system lines may span hundreds of miles, a key difficulty in power system restoration is determining the location of the fault

One newer technique is the use of the global positioning system (GPS).

GPS can provide time synchronization of about 1 microsecond

Since the traveling electromagnetic waves propagate at about the speed of light (300m per microsecond), the fault location can be found by comparing arrival times of the waves at each substation