ece 476 power system analysis lecture 25: transient stability, geomagnetic disturbances prof. tom...

44
ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering University of Illinois at Urbana- Champaign [email protected]

Upload: augustus-webster

Post on 21-Jan-2016

233 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

ECE 476 Power System Analysis

Lecture 25: Transient Stability, Geomagnetic Disturbances

Prof. Tom Overbye

Dept. of Electrical and Computer Engineering

University of Illinois at Urbana-Champaign

[email protected]

Page 2: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Announcements

• Read Chapters 11 and 12 (sections 12.1 to 12.3)• Homework 11is 11.19, 11.25, 12.3, 12.11, 14.15; it

should be done before the final but is not to be turned in

• Design project due today• Final exam is Wednesday Dec 16, 7 to 10pm,

room 1013; comprehensive, closed book, closed notes with three note sheets and standard calculators allowed

2

Page 3: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Generator Governors

• The other key generator control system is the governor, which changes the mechanical power into the generator to maintain a desired speed and hence frequency.

• Historically centrifugal “flyball” governors have been used to regulate the speed of devices such as steam engines

• The centrifugal force varieswith speed, opening orclosing the throttle valve

Photo source: en.wikipedia.org/wiki/Centrifugal_governor3

Page 4: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Isochronous Governors

• Ideally we would like the governor to maintain the frequency at a constant value of 60 Hz (in North America)

• This can be accomplished using an isochronous governor. • A flyball governor is not an isochronous governor since

the control action is proportional to the speed error• An isochronous governor requires an integration of the

speed error

• Isochronous governors are used on stand alone generators but cannot be used on interconnected generators because of “hunting”

4

Page 5: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Generator “Hunting”

• Control system “hunting” is oscillation around an equilibrium point

• Trying to interconnect multiple isochronous generators will cause hunting because the frequency setpoints are the two generators are never exactly equal• One will be accumulating a frequency error trying to

speed up the system, whereas the other will be trying to slow it down

• The generators will NOT share the power load proportionally.

5

Page 6: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Droop Control

• The solution is to use what is known as droop control, in which the desired set point frequency is dependent upon the generator’s output

1m refp p f

R

R is known as the regulation constantor droop; a typicalvalue is 4 or 5%.

6

Page 7: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Governor Block Diagrams

• The block diagram for a simple stream unit, the TGOV1 model, is shown below. The T1 block models the governor delays, whereas the second block models the turbine response.

maxV

1

1

1 sT

minV

1

R

tD

2

3

1

1

sT

sT

refP mechP

ΔωSpeed

7

Page 8: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Example 12.4 System Response

8

Page 9: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Problem 12.11

slack

SLACK345

SLACK138

RAY345

RAY138

RAY69

FERNA69

A

MVA

DEMAR69

BLT69

BLT138

BOB138

BOB69

WOLEN69

SHI MKO69

ROGER69

UI UC69

PETE69

HI SKY69

TI M69

TI M138

TI M345

PAI 69

GROSS69

HANNAH69

AMANDA69

HOMER69

LAUF69

MORO138

LAUF138

HALE69

PATTEN69

WEBER69

BUCKY138

SAVOY69

SAVOY138

J O138 J O345

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

A

MVA

1.02 pu

1.01 pu

1.02 pu

1.03 pu

1.01 pu

1.00 pu1.00 pu

0.99 pu

1.02 pu

1.01 pu

1.00 pu

1.01 pu1.01 pu

1.01 pu

1.01 pu

1.02 pu

1.00 pu

1.00 pu

1.02 pu

0.997 pu

0.99 pu

1.00 pu

1.02 pu

1.00 pu1.01 pu

1.00 pu

1.00 pu 1.00 pu

1.01 pu

1.02 pu 1.02 pu

1.02 pu 1.03 pu

A

MVA

1.02 pu

A

MVA

A

MVA

LYNN138

A

MVA

1.02 pu

A

MVA

1.00 pu

A

MVA

218 MW 54 Mvar

21 MW 7 Mvar

45.3 MW 12 Mvar

140 MW 45 Mvar

37 MW

13 Mvar

12 MW 5 Mvar

150 MW -0 Mvar

56 MW

13 Mvar

15 MW 5 Mvar

14 MW

2 Mvar

42 MW 2 Mvar

45 MW 0 Mvar

58.2 MW 36 Mvar

36 MW 10 Mvar

0 MW 0 Mvar

22 MW 15 Mvar

60 MW 12 Mvar

20 MW 30 Mvar

23 MW 7 Mvar

33 MW 13 Mvar

16.0 Mvar 18 MW 5 Mvar

58 MW 40 Mvar 51 MW

15 Mvar

14.3 Mvar

33 MW 10 Mvar

15 MW 3 Mvar

23 MW 6 Mvar 14 MW

3 Mvar

4.8 Mvar

7.2 Mvar

12.8 Mvar

29.0 Mvar

7.4 Mvar

0.0 Mvar

106 MW 8 Mvar

20 MW 8 Mvar

150 MW -0 Mvar

17 MW 3 Mvar

0 MW 0 Mvar

14 MW 4 Mvar

20191817161514131211109876543210

60

59.98

59.96

59.94

59.92

59.9

59.88

59.86

59.84

59.82

59.8

59.78

59.76

59.74

59.72

59.7

59.68

59.66

9

Page 10: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Restoring Frequency to 60 Hz

• In an interconnected power system the governors to not automatically restore the frequency to 60 Hz

• Rather this is done via the ACE (area control area calculation). Previously we defined ACE as the difference between the actual real power exports from an area and the scheduled exports. But it has an additional termACE = Pactual - Psched – 10b(freqact - freqsched)

• b is the balancing authority frequency bias in MW/0.1 Hz with a negative sign. It is about 0.8% of peak load/generation

10

Page 11: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

2600 MW Loss Frequency Recovery

Frequency recovers in about ten minutes

Page 12: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

2007 CWLP Dallman Accident

• In 2007 there was an explosion at the CWLP 86 MW Dallman 1 generator. The explosion was eventually determined to be caused by a sticky valve that prevented the cutoff of steam into the turbine when the generator went off line. So the generator turbine continued to accelerate up to over 6000 rpm (3600 normal). – High speed caused parts of the generator to shoot out– Hydrogen escaped from the cooling system, and

eventually escaped causing the explosion– Repairs took about 18 months, costing more than $52

million12

Page 13: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Dallman After the Accident

13

Page 14: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Outside of Dallman

14

Page 15: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

High-Impact, Low-Frequency Events

• In 2010 the North American Electric ReliabilityCorporation (NERC) identified some severe grid threads called High-Impact, Low-Frequency Events (HILFs); others call them blackswan events or black sky days– Large-scale, potentially long duration blackouts

• HILFs identified by NERC were 1. a coordinated cyber, physical or blended attacks,

2. pandemics,

3. geomagnetic disturbances (GMDs), and

4. high altitude electromagnetics pulses (HEMPs)

15

Page 16: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Geomagnetic Disturbances (GMDs)

• GMDs are caused by corona mass ejections (CMEs) from the sun; a GMD caused the Quebec blackout in 1989

• They have the potential to severely disrupt the electric grid by causing quasi-dc geomagnetically induced currents (GICs) in the high voltage grid

• Until recently power engineers had few tools to help them assess the impact of GMDs

• GMD assessment tools are now moving into the realm of power system planning and operations engineers

• Wide industry interest in GMD assessment

16

16

Page 17: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

In the News: National Space Weather Action Plan

• On 10/28/15 the White House released the National Space Weather Action Plan– Quoting from the Introduction, “Given the importance of

reliable electric power and space-based assets, it is essential that the United States has the ability to protect, mitigate, respond to, and recover from the potentially devastating effects of space weather.”

• Plan structure includes – 1) Establish Benchmarks, 2) Enhance Response and Recovery

Capabilities, 3) Improve Protection and Mitigation Efforts, 4) Improve Assessment, Modeling, and Prediction of Impacts on Critical Infrastructure, 5) Improve Space-Weather Services, 6) Increase International Cooperation

17

Page 18: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Analysis Requires Consideration of Several Time Frames

Image: Sauer, P.W., M. A. Pai, Power System Dynamics and Stability, Stripes Publishing, 2007

GMDs impact grid on time scale of many seconds to hours, quasi-steady state analyzed by power flow

18

Page 19: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Quick Demo of How the Grid Can Fail in the Power Flow Time Frame

19

Page 20: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GMD Overview

• Solar corona mass ejections (CMEs) can cause changes in the earth’s magnetic field (i.e., dB/dt). These changes in turn produce a non-uniform electric fields– Changes in the magnetic flux are usually expressed in

nT/minute; from a 60 Hz perspective they produce an almost dc electric field

– 1989 North America storm produced a change of 500 nT/minute, while a stronger storm, such as the ones in 1859 or 1921, could produce 5000 nT/minute variation

– Storm “footprint” can be continental in scale– Earth’s magnetic field is normally between 25,000 and 65,000

nT, with higher values near the poles

Image source: J. Kappenman, “A Perfect Storm of Planetary Proportions,” IEEE Spectrum, Feb 2012, page 29 20

Page 21: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Electric Fields and Geomagnetically Induced Currents (GICs)

• The induced electric field at the surface is dependent on deep earth (hundreds of km) conductivity– Electric fields are vectors (magnitude and angle); values

expressed in units of volts/mile (or volts/km);– A 2400 nT/minute storm could produce 5 to 10 volts/mile.

• The electric fields cause GICs to flow in the high voltage transmission grid

• The induced voltages that drive the GICs can be modeled as dc voltages in the transmission lines. – The magnitude of the dc voltage is determined by integrating

the electric field variation over the line length– Both magnitude and direction of electric field is important

21

Page 22: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

July 2012 GMD Near Miss

• In July 2014 NASA said in July of 2012 there was a solar CME that barely missed the earth– It would likely have

caused the largestGMD that we haveseen in the last 150years

• There is still lots of uncertainly about how large a storm is reasonable to consider in electric utility planning

Image Source: science.nasa.gov/science-news/science-at-nasa/2014/23jul_superstorm/ 22

Page 23: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Geomagnetically Induced Currents (GICs

• GMDs cause slowly varying electric fields• Along length of a high voltage transmission line,

electric fields can be modeled as a dc voltage source superimposed on the lines

• These voltage sources produce quasi-dc geomagnetically induced currents (GICs) that are superimposed on the ac (60 Hz) flows

23

Page 24: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Transformer Impacts of GICs

• The superimposed dc GICscan push transformers into saturation part of the cycle

• This can cause large harmonics; in the positive sequence (e.g., power flow and transient stability) these harmonics can be represented by increased reactive power losses in the transformer

Images: Craig Stiegemeier and Ed Schweitzer, JASON Presentations, June 2011

Harmonics

24

Page 25: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GMD Enhanced Power Analysis Software

• By integrating GIC calculations directly within power flow and transient stability engineers can see the impact of GICs on their systems, and consider mitigation options

• GIC calculations use many of the existing model parameters such as line resistance. Some non-standard values are also needed; either provided or estimated– Substation grounding resistance– transformer grounding configuration, transformer coil

resistance, whether auto-transformer, whether three-winding transformer,

– generator step-up transformer parameters25

Page 26: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Overview of GMD Assessments

Image Source: http://www.nerc.com/pa/Stand/WebinarLibrary/GMD_standards_update_june26_ec.pdf

The two key concerns from a big storm are 1) large-scaleblackout due to voltage collapse, 2) permanent transformer damage due to overheating

In is a quite interdisciplinary problem

26

Page 27: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Four Bus Example

,3

150 volts93.75 amps or 31.25 amps/phase

1 0.1 0.1 0.2 0.2GIC PhaseI

The line and transformer resistance and current values are per phase so the total current is three times this value. Substation grounding values are total resistance. Brown arrows show GIC flow.

27

Page 28: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Determining GMD Storm Scenarios

• The starting point for the GIC analysis is an assumed storm scenario; determines the line dc voltages

• Matching an actual storm can be complicated, and requires detailed knowledge of the associated geology

• GICs vary linearly with the assumed electric field magnitudes and reactive power impacts on the transformers is also mostly linear

• Working with space weather community to determine highest possible storms

• NERC proposed a non-uniform field magnitude model that FERC has partially accepted (FERC has been seeking industry comments in summer of 2015) 28

Page 29: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Power Flow Embedded GIC Calculations: The G Matrix

• With knowledge of the pertinent transmission system parameters and the GMD-induced line voltages, the dc bus voltages and flows are found by solving a linear equation

I = G V

– The G matrix is similar to the Ybus except 1) it is augmented to include substation neutrals, and 2) it is just resistive values (conductances)

– The current vector contains the Norton injections associated with the GMD-induced line voltages

• Factoring the sparse G matrix is fast!29

Page 30: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

G Matrix Considerations

•Data needed at least for the study footprint & neighbors• Transmission line resistance values are readily

obtained from the power flow cases• DC resistance is quite close to ac values; temperature dependence (0.4%

per degree C) plays a role

• Estimates of transformer winding resistance can be obtained from the power flow cases– Usually whether they are auto-transformers can be

determined– Whether device is a three winding transformer can usually be

guessed (if not explicitly modeled)

• Substation grounding values needed30

Page 31: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Input Electric Field Considerations

• The current vector (I) depends upon the assumed electric field along each transmission line

• With a uniform electric field determination of the transmission line’s GMD-induced voltage is path independent– Just requires geographic knowledge of the transmission line’s

terminal substations

• With nonuniform fields an exact calculation would be path dependent, but just a assuming a straight line path is probably sufficient (given all the other uncertainties!)

31

Page 32: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

EPRI Small 20 Bus Benchmark System Example

32

Page 33: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Assumed Geographic Location (Mostly East-West)

33

Page 34: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Flows with a 1V/km North-South, Uniform Electric Field

slack

17 16

23

15

4

205

6

11

12

18

19

1

7

8

13 14

900 MW 95 Mvar

900 MW 95 Mvar

500 MW

17 Mvar 500 MW 17 Mvar

600 MW

121 Mvar

600 MW

121 Mvar

779 MW

100 Mvar

900 MW

400 Mvar

1200 MW

350 Mvar

1200 MW

500 Mvar

Substation 2

Substation 1

Substation 3

Substation 4

Substation 5

Substation 6

Substation 8 21

500 MW 200 Mvar

Total GIC Losses 528.9 Mvar

536.8 Mvar

204.3 Mvar

300 MW 150 Mvar

600 MW

200 Mvar

34

Page 35: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Flows with a 1V/km East-West, Uniform Electric Field

slack

17 16

23

15

4

205

6

11

12

18

19

1

7

8

13 14

900 MW 181 Mvar

900 MW 181 Mvar

500 MW

31 Mvar 500 MW 31 Mvar

600 MW

131 Mvar

600 MW

131 Mvar

779 MW

118 Mvar

900 MW

400 Mvar

1200 MW

350 Mvar

1200 MW

500 Mvar

Substation 2

Substation 1

Substation 3

Substation 4

Substation 5

Substation 6

Substation 8 21

500 MW 200 Mvar

Total GIC Losses 758.3 Mvar

532.8 Mvar

205.0 Mvar

300 MW 150 Mvar

600 MW

200 Mvar

35

Page 36: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Flows with a 2V/km East-West, Uniform Electric Field

slack

17 16

23

15

4

205

6

11

12

18

19

1

7

8

13 14

900 MW 400 Mvar

900 MW 400 Mvar

500 MW

113 Mvar 500 MW 113 Mvar

600 MW

300 Mvar

600 MW

300 Mvar

786 MW

198 Mvar

900 MW

400 Mvar

1200 MW

350 Mvar

1200 MW

500 Mvar

Substation 2

Substation 1

Substation 3

Substation 4

Substation 5

Substation 6

Substation 8 21

500 MW 200 Mvar

Total GIC Losses 1474.9 Mvar

493.2 Mvar

189.4 Mvar

300 MW 150 Mvar

600 MW

200 Mvar

36

Page 37: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Flows with a 2.2V/km East-West, Uniform Electric Field – Near Voltage Collapse

slack

17 16

23

15

4

205

6

11

12

18

19

1

7

8

13 14

900 MW 400 Mvar

900 MW 400 Mvar

500 MW

172 Mvar 500 MW 172 Mvar

600 MW

389 Mvar

600 MW

389 Mvar

792 MW

251 Mvar

900 MW

400 Mvar

1200 MW

350 Mvar

1200 MW

500 Mvar

Substation 2

Substation 1

Substation 3

Substation 4

Substation 5

Substation 6

Substation 8 21

500 MW 200 Mvar

Total GIC Losses 1587.5 Mvar

463.9 Mvar

179.3 Mvar

300 MW 150 Mvar

600 MW

200 Mvar

37

Page 38: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

The Impact of a Large GMD From an Operations Perspective

• Would be maybe a day warning but without specifics – Satellite at Lagrange point one million miles from earth would

give more details, but with just 30 minutes before impact– Would strike quickly; rise time of minutes, rapidly covering a

good chunk of the continent

• Reactive power loadings on hundreds of transformers could sky rocket, causing heating issues

• Power system software like state estimation could fail• Control room personnel would be overwhelmed• The storm could last for days with varying intensity• Waiting until it occurs to prepare is not a good idea

38

Page 39: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Transient Stability Level GMD Impact Simulation

The interactive simulation shows a GMD induced voltagecollapse scenario with some protection system modeling

39

Page 40: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Flows in Eastern Interconnect for a Uniform 8.0 V/km, East-West Field

40

40

Page 41: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Geographic Data Views: Displaying Net Substation Current Injections

41

GICs tend to concentrate at network boundaries

41

Page 42: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Power Flow Convergence Issues

• Integrated GIC modeling can certainly impact power flow convergence since the GIC induced reactive power losses simultaneously add lots of reactive power.

• Several techniques can help prevent divergence– Just calculating the GICs without solving the power flow– Gradually increasing the assumed electric fields to avoid

simultaneously adding too much reactive power– Only calculating the GIC transformer reactive power losses

for specified areas; reactive power doesn’t travel far– Freezing reactive control devices such as LTC taps– Solving in transient stability

42

42

Page 43: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

GIC Mitigation

• Engineers need tools to determine mitigation strategies– Cost-benefit analysis

• GIC flows can be reduced both through operational strategies such as opening lines, and through longer term approaches such as installing blocking devices

• Redispatching the system canchange transformer loadings,providing margins for GICs

• Algorithms are needed to provide power engineers with techniques that go beyond trial-and-error

43

43

Photo from ATC

Page 44: ECE 476 Power System Analysis Lecture 25: Transient Stability, Geomagnetic Disturbances Prof. Tom Overbye Dept. of Electrical and Computer Engineering

Research Directions

• We’ve made good progress, but still much to do!• GMD/GIC validation: While large GMDs are rare,

small ones occur regularly; magnetometers, transformer neutral current measurements and PMUs are providing the information needed for better validation

• GIC sensitivity analysis: which parameters are most important, how large of system models

• How can GICs be effectively mitigated

• Much of GIC analysis also applies to EMP E3 though on the shorter transient stability time scale

44

44