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Phasor-Only State Estimation Ali Abur Department of Electrical and Computer Engineering Northeastern University, Boston [email protected] PSERC Webinar October 7, 2014

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Page 1: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-Only State Estimation

Ali AburDepartment of Electrical and Computer Engineering

Northeastern University, [email protected]

PSERC WebinarOctober 7, 2014

Page 2: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

2

Page 3: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Background and terminology

(Static) state estimationMeasurement type: SCADA / SynchrophasorFormulation: Nonlinear / Linear Network model: + sequence / 3-phase

Dynamic state estimationWide-area, using gen/load/network variablesLocal, using gen variables, boundary measurements or estimates

3

Page 4: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Modeling

Gen1

Gen2

GenNG

Load 1 Load 2

Load NL

Transmission Network[Lines + Transformers]

Measurements4

Page 5: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Modeling [ SSE ]

Gen1

Gen2

GenNG

Load 1 Load 2

Load NL

Transmission Network[Lines + Transformers]

Estimated Measurements

SSE: Estimation of the snap-shotat time “t”

Linear or NLPos Seq or 3-PhaseSCADA or Phasor orMixed SCADA/Phasor

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Page 6: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Modeling [ DSE ]

Gen1

Gen2

GenNG

Load 1 Load 2

Load NL

Transmission Network[Lines + Transformers]

Estimated Measurements

DSE: Single machine / zonal / wide-areaDetailed Gen and Load models Frequency and power angle estimation

Zone-2

Zone-1

Zone NZ

Tracking the network anddynamic gen/load statevariables in real-time

6

Page 7: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Timeline

[z(t)]

�𝑋𝑋 𝑡𝑡�̂�𝛿 𝑡𝑡�𝜔𝜔(𝑡𝑡)

�̂�𝑧𝑔𝑔 𝑡𝑡𝑡

�̂�𝛿 𝑡𝑡𝑡�𝜔𝜔(𝑡𝑡𝑡)

𝑡𝑡 𝑡𝑡𝑡 𝑡𝑡 + 𝑑𝑑𝑡𝑡 𝑡𝑡 + 2𝑑𝑑𝑡𝑡 𝑡𝑡 + 3𝑑𝑑𝑡𝑡 𝑡𝑡 + 4𝑑𝑑𝑡𝑡

DSE / Local

SSE /Wide-area

DSE /Wide-area

SSE

DSE

7

Page 8: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Timeline

[z(t)]

�𝑋𝑋 𝑡𝑡�̂�𝛿 𝑡𝑡�𝜔𝜔(𝑡𝑡)

�̂�𝑧𝑔𝑔 𝑡𝑡𝑡

�̂�𝛿 𝑡𝑡𝑡�𝜔𝜔(𝑡𝑡𝑡)

𝑡𝑡 𝑡𝑡𝑡 𝑡𝑡 + 𝑑𝑑𝑡𝑡 𝑡𝑡 + 2𝑑𝑑𝑡𝑡 𝑡𝑡 + 3𝑑𝑑𝑡𝑡 𝑡𝑡 + 4𝑑𝑑𝑡𝑡

DSE / Local

SSE /Wide-area

DSE /Wide-area

DSE

8

Page 9: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

9

Page 10: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Static state estimation:Objective and measurements

Objective: To obtain the best estimate of the state of the system based on a set of measurements.

– State variables: voltage phasors at all buses in the system – Measurements:

• Power injection measurements • Power flow measurements• Voltage/Current magnitude measurements• Synchronized phasor measurements

SCAD

AM

easu

rem

ents

Introduced by Schweppe and his co-workers in 1969.

Schweppe, F.C., Wildes, J., and Rom, D., “Power system static state estimation: Parts I, II, III”, Power Industry Computer Applications (PICA), Denver, CO, June 1969.

10

Page 11: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

State estimation: data/info flow diagram• Topology Processor• Network Observability Analysis• WLS State Estimator• Bad Data Processor• Parameter and Topology Error Processor

Analog MeasurementsPi, Qi, Pf, Qf, V, I

Topology Processor

State Estimator

Network Observability Check

V, θ Bad Data Processor

Network Parameters, Branch Status, Substation Configuration

Parameter and Topology Errors Detection, Identification,

Correction

Load ForecastsGeneration Schedules

PM +

11

Page 12: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

• Topology Processor• Network Observability Analysis• Robust LAV State Estimator• Bad Data Processor• Parameter and Topology Error Processor

Analog MeasurementsPi, Qi, Pf, Qf, V, I

Topology Processor

State Estimator

Network Observability Check

V, θ Bad Data Processor

Network Parameters, Branch Status, Substation Configuration

Parameter and Topology Errors Detection, Identification,

Correction

Load ForecastsGeneration Schedules

State estimation: data/info flow diagram

PM +

12

Page 13: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

13

Page 14: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor measurement units (PMU)

“Synchronized Phasor Measurements and Their Applications” by A.G. Phadke and J.S. Thorp

Invented by Professors Phadke and Thorp in 1988.

They calculate the real-time phasor measurements synchronized to an absolute time reference provided by the Global Positioning System.PMUs facilitate direct measurement of phase angle differences between remote bus voltages in a power grid.

14

Page 15: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor Measurement Units (PMU)Phasor Data Concentrators (PDC)[*]

GPS CLOCK

AntennaPMU 1

PT

CT

PDC

[*] IEEE PSRC Working Group C37 Report

CORPORATEPDC

REGIONALPDC

DATA STORAGE& APPLICATIONS

DATA STORAGE& APPLICATIONS

PMU 2

PMU 3

PMU 4PMU K

15

Page 16: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Taken verbatim from: IEEE C37.244-2013 PDC Guide

PDC Definition:A function that collects phasor data, and discrete eventdata from PMUs and possibly from other PDCs, andtransmits data to other applications.

PDCs may buffer data for a short time period, but do notstore the data. This guide defines a PDC as a functionthat may exist within any given device.

Phasor Data Concentrator (PDC)

16

Page 17: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor voltage measurements

Reference

17

Page 18: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Reference phasor

+ϴ1

--ϴ2

--ϴ3 +ϴ1

--ϴ2

--ϴ3

Reference

Reference

18

Page 19: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

US Energy Information Administration: http://www.eia.gov/todayinenergy/detail.cfm?id=5630

Under the Recovery Act SGIG and SGDP programs, their numbers rapidly increased : 166 1126

19

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Measurements provided by PMUs

PMUV phasor

I phasors

ALL 3-PHASES ARE TYPICALLY MEASUREDBUTONLY POSITIVE SEQUENCE COMPONENTS ARE REPORTED

𝑉𝑉𝐴𝐴𝑉𝑉𝐵𝐵𝑉𝑉𝐶𝐶

= [𝑇𝑇]𝑉𝑉0𝑉𝑉+𝑉𝑉−

𝑉𝑉+ = 13[𝑉𝑉𝐴𝐴+∝ 𝑉𝑉𝐵𝐵+∝2 𝑉𝑉𝐶𝐶]

∝= 𝑒𝑒𝑗𝑗2𝜋𝜋3

20

Page 21: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

21

Page 22: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Measurement equations

onlyparametersnetworkofFunctionHModelLinearXHZ

tsMeasuremenPhasorXhH

ModellinearNonXhZtsMeasuremenSCADA

x

:

)(:)(

υ

υ

+⋅=

∇−+=

A.G. Phadke, J.S. Thorp, and K.J. Karimi, “State Estimation with Phasor Measurements”, IEEE Transactions on Power Systems, vol. 1, no.1, pp. 233-241, February 1986.

22

Page 23: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellationsLAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

23

Page 24: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation

varianceerroriiRERHRHG

solutionDirectZRHGX

sidualrXHZrtoSubject

rMinimize

problemestimationstateWLSModelLinearXHZ

i

TT

T

m

i i

i

),(:)cov(}{;

ˆ

:

2

1

11

2

2

σ

υυυ

σ

υ

=⋅==

=

⋅−=

+⋅=

−−

24

Page 25: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation

[ ]

matrix incidence bus-branch :matrix admittancebranch :

matrixidentity :

AYU

VAY

U

currentsBranchvoltagesBus

IV

Z

b

b

m

mm

υ+⋅

=

⇒⇒

=

Consider a fully measured system:

Note: Shunt branches are neglected initially, they will be introduced later.25

Page 26: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation

[ ]

[ ] [ ] υ

υ

++⋅=

++⋅

⋅+

=

++

=

jfeH

jfeAjbg

U

jdcjfe

IV

Let

F

mm

mm

m

m

)(

26

Page 27: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation:Complex to real transformation

[ ] υ

υ

+

⋅=

+

−=

fe

HZ

fe

gAbAbAgA

UU

dcfe

m

m

m

m

][

27

Page 28: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation:Exact cancellations in off-diagonals of [G]

( )( )

++++

=

−⋅

−=⋅=

AggbbAUAbbggAU

gAbAbAgA

UU

gAbAbAgA

UU

HHG

TTT

TTT

T

T

00

[G] matrix:• Is block – diagonal• Has identical diagonal blocks• Is constant, independent of the state

R is assumed to be identity matrix without loss of generality

28

Page 29: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Phasor-only WLS state estimation:Correction for shunt terms

XHRHGX

XHZRHGX

ZRHGXXE

XEHuEXHu

uXHXHHZ

shT

shTcorr

T

sh

sh

sh

ˆˆ)ˆ(

ˆ}{

}{}{

)(][

11

11

11

⋅−=

⋅−=

==

⋅=+⋅=

+⋅=+⋅+=

−−

−−

−−

υυ

Very sparse

29

Page 30: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Fast Decoupled WLS Implementation Results

Test Systems Used

SystemLabel

Number of Buses

Number of Branches

Number of Phasor

Measurements

A 159 198 222

B 265 340 361

C 3625 4836 4982

Case-1: No bad measurement.Case-2: Single bad measurement.Case-3: Five bad measurements.

Cases simulated:

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System CaseMSE

WLS Decoupled WLS

A1 0.59 0.592 0.59 0.593 0.62 0.62

B1 0.61 0.612 0.61 0.603 0.62 0.63

C1 0.59 0.592 0.58 0.593 0.58 0.59

Average MSE Values ( for 100 Simulations)

Fast Decoupled WLS Implementation Results

31

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MEAN CPU TIMES OF 100 SIMULATIONS

System CaseCPU Times (ms)

WLS Decoupled WLS

A1 5 2.42 5.7 2.73 9.3 3.9

B1 7.5 3.52 8.7 3.93 14.8 5.8

C1 137.4 75.92 169.5 95.73 284.7 165.6

Fast Decoupled WLS Implementation Results

32

Page 33: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

33

Page 34: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

L1 (LAV) Estimator

]1,,1,1[

ˆ

||1

=

+⋅=

⋅∑=

T

m

i

T

crXHZtoSubject

rcMinimize

Robust but with known deficiency:Vulnerable to leverage measurements

34

Page 35: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

No leverage pointsL1 estimator successfully rejects bad data

Motivating example: simple regression

Wrong data

x

y y

35

Page 36: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Leverage point exists and contains gross error:L1 estimator fails to reject bad measurement

Wrong data(leverage point)

Motivating example: simple regression

y

x

36

Page 37: Phasor-Only State Estimation · 10/7/2014  · Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358. 1 − = x x x Y Y Y x x x x x x x x x x

Leverage points in measurement model

– Flow measurements on the lines with impedances, which are very different from the rest of the lines.

– Using a very large weight for a specific measurement.

Mili L., Cheniae M.G., and Rousseeuw P.J., “Robust State Estimation of Electric Power Systems” IEEE Transactions on Circuits and Systems, Vol. 41, No. 5, May 1994, pp.349-358.

1

=−

xxxYYYxxxxxxxxxxxx

HRLEVERAGEMEASUREMENT

zexH =+

Scaling both the measured value and the measurement jacobian row will eliminate leveraging effect of the measurement.

Leave zero injections since they are error free by design.Incorporate equality constraints in the formulation.

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Properties of L1 estimator• Efficient Linear Programming (LP) code exists

to solve it for large scale systems.• Use of simple scaling eliminates leverage

points. This is possible due to the type of phasor measurements (either voltages or branch currents).

• L1 estimator automatically rejects bad data given sufficient local redundancy, hence bad data processing is built-in.

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Conversion to Equivalent LP Problem

zrHxtsrT

=+ ..||c min

0 ..

c min

≥=

yzMyts

yT

][][

]00[c

IIHHMVUXXy

ccTTTT

bTa

mmnnT

−−==

=

VUrXXx ba

−=

= -

39

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Bad data processing

LP problem is solved once. Choice of initial basis impacts solution time/iterations.

Update the estimates

Normalized Residuals Test (NRT):

NRT is repeated as many times as the number of bad data.

WLS: Post estimation bad data processing / re-estimation

L1: Linear Programming Solution

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Small system exampleIEEE 30-bus system

Line 1-2 parameter is changed to transform 𝐼𝐼1−2into a leverage measurement

Case 1: Base case true solution

Case 2: Bad leverage measurement without scaling

Case 3: Same as Case 2, but using scaling

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Case-1 Case-2 Case-3

V (pu) θ (deg) V (pu) θ (deg) V (pu) θ (deg)

1 1 5.2 1.0118 -3.5462 1 5.2

2 1 -3.74 0.9999 -3.74 1 -3.74

3 0.9952 0.13 1.004 -3.8964 0.9952 0.13

4 0.9992 -4.81 0.9992 -4.81 0.9992 -4.81

5 1 -9.02 0.9999 -9.02 1 -9.02

6 0.9851 -7.41 0.9851 -7.41 0.9851 -7.41

7 0.9869 -8.88 0.9869 -8.88 0.9869 -8.88

Small system exampleBase caseTrue Solution Leverage Measurements

Bad dataNo scaling

Leverage MeasurementsBad dataWith scaling

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Large test case: 3625 bus + 4836 branch utility system

Case a: No bad measurement.Case b: Single bad measurement.Case c: Five bad measurements.

Case a Case b Case c

LAV 3.33 s. 3.36 s. 3.57 s.

WLS 2.32 s. 9.38 s. 50.2 s.

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Phasor-only state estimation:WLS versus L1 (LAV)

WLS :– Linear solution– Requires bad-data analysis

– Normalized residuals test– Re-weighting (not applicable)

– No deficiency in the presence of leverage measurements, with scaling.

– Exact cancellations in [G]

L1 (LAV):– Linear programming (single solution)

computationally competitive in s-s– Does not require bad-data analysis[*]

– No deficiency in the presence of leverage measurements, with scaling.

[*] Kotiuga W. W. and Vidyasagar M., “Bad Data Rejection Properties of Weighted Least Absolute Value Techniques Applied to Static State Estimation,” IEEE Transactions on Power Apparatus and Systems, Vol. PAS-101, No. 4, April 1982, pp. 844-851.

44

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Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

45

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3-phase operation:motivation and observations

• State estimators implicitly assume balanced operating conditions and use positive sequence network model and measurements. This assumption is sometimes questionable.

• Power measurements are non-linear functions of state variables.

• Phasor measurements are linearly related to the states.

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Further motivation• Develop a state estimator capable of solving

state estimation for three-phase unbalanced operating conditions,

yet:• Utilize existing, well developed and tested

software as much as possible.

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Proposed approach:Modal decomposition revisited

• Decompose phasor measurements into their symmetrical components

• Estimate individual symmetrical components of states separately ( in parallel if such hardware is available )

• Transform the estimates into phase domain to obtain estimated phase voltages and flows.

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Modal decomposition ofmeasurement equations

eHVZ +=

][ TI

TV

T ZZZ =

PS TVV = PS TII =

=

T

TT

TZ

000

000

eTHVTZT ZZZ +=

Phasor domain measurement representationH: 3mx3nV: 3nx1Z: 30x1

&Modal domain vectorsT: 3x3VS and IS: 3x1

T: 3mx3m

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=−

1

1

1

000

000

T

TT

TV

MVVTV =

MMMM eVHZ +=

eTeHTTHZTZ

ZM

VZM

ZM

===

0000 eVHZ += rrrr eVHZ +=

01

001

00 ZRHGV T −−= rrTrrr ZRHGV 11 −−=

01

000 HRHG T −=

Zero sequence Positive/ Negative sequence

Z0, Zr : mx1V0, Vr: nx1H0, Hr: mxn!

rrTrr HRHG 1−=

•Fully decoupled three relations •Smaller size (Jacobian) matrices

Modal decomposition ofmeasurement equations

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Large scale 3-phase system example:3625-buses and 4836-branches

Case a Case b Case c

LAV WLS LAV WLS LAV WLS

Zero Seq. 3.52 s. 2.32 s. 3.65 s. 9.28 s. 3.78 s. 25.51 s.

Positive Seq. 3.61 s. 2.62 s. 3.63 s. 9.41 s. 3.66 s. 26.01 s.

Negative Seq. 3.21 s. 2.22 s. 3.45 s. 9.01 s. 3.62 s. 24.82 s.

Case a: No bad measurement.Case b: Single bad measurement.Case c: Five bad measurements.

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Talk Outline

Background and terminologyState estimationPhasor measurementsPhasor-only state estimation

WLS: exact cancellations LAV: improved robustness Extension to 3-phase networks

Observability and error identificationClosing remarks

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No reference bus or reference PMUis needed or should be used

• Eliminate the reference phase angle from the SE formulation.

• Bad data in SCADA as well as phasor measurements can be detected and identified with sufficiently redundant measurement sets.

PMUMeas.

SCADAMeas.

State

Estimator &

Bad Data

Processor

Estimated/CorrectedPMU&SCADA Meas.

Estimated State

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Numerical Example

: Power Injection : Power Flow : Voltage Magnitude

: PMU54

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Numerical ExampleError in bus 1 phase angle

TEST ABus 1 is used as the reference bus

TEST BNo reference is used

MeasurementNormalized

residual MeasurementNormalized

residual7.5 10.535.73 7.25.6 5.485.2 5.354.53 4.96

Test A Test B

8θ 1θ

74−p 8θ

65−p 74−p12θ 65−p1V 12θ

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Merging Observable Islands

• PMUs can be placed at any bus in the observable island.

• SCADA pseudo-measurements can merge observable islands only if they are incident to the boundary buses.

PP

SS

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Robust Metering

• Bad data appearing in “critical measurements” can NOT be detected.

• Adding new measurements at strategic locations will transform them, allowing detection of bad data which would otherwise have been missed.

Note:When a “critical measurement” is removed from the measurement set, the network will no longer be OBSERVABLE.

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IEEE 57-bus systemCriticalMeas.

Type

1 F41-43

2 F36-35

3 F42-41

4 F40-56

5 I-11

6 I-24

7 I-39

8 I-37

9 I-46

10 I-48

11 I-56

12 I-57

13 I-34

P

P

Number of Critical Meas. Number of PMU needed

13 2

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IEEE 118-bus systemNumber of Critical Meas. Number of PMU needed

29 13

P

P

P

P

P

P

P

P

P

P

P

P

P

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Impact of PMUs onParameter Error Identification

• Are there cases where errors in certain parameters can not be identified without synchronized phasor measurements?

Cases where more than one set of parameters satisfies all SCADA measurements.

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Illustrative Example

),,(),,( 2121 ppxJppxJ ′′′=

k lkl

kl

Px

θ θ−=

lm

mllm x

P′

−′=

θθ

' 'kl k l

kl k l

xx

θ θθ θ

−=

−' 'lm l m

lm l m

xx

θ θθ θ

−=

l mlm

lm

Px

θ θ−=

kl

lkkl x

P′

′−=

θθ

Pl=Plm - Pkl

Vk Vl

Vm61

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Illustrative Example

),,(),,( 2121 ppxJppxJ ′′′=

k lkl

kl

Px

θ θ−=

lm

mllm x

P′

−′=

θθ

' 'kl k l

kl k l

xx

θ θθ θ

−=

−' 'lm l m

lm l m

xx

θ θθ θ

−=

l mlm

lm

Px

θ θ−=

kl

lkkl x

P′

′−=

θθ

Pl=Plm - Pkl

Vk

Vl’

Vm62

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Remarks and Conclusions

• LAV estimator will be a computationally viable and effective alternative to WLS estimator when the measurement set consists of only PMUs. Scaling can be a simple yet effective tool in the presence of leverage measurements.

• Use of phasor measurements for SE allows modal decomposition of measurement equations.

• WLS estimator implementation has built-in simplifications due to exact cancellations in the gain [G] matrix.

• Given sufficiently redundant phasor measurements, fast and robust state estimation is possible even for very large scale power grids.

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Related Publications:

Göl, M. and Abur, A., “A Hybrid State Estimator for Systems with Limited Number of PMUs,” accepted for publication in IEEE Transactions on Power Systems, 2014.

Göl, M. and Abur, A., “LAV Based Robust State Estimation for Systems Measured by PMUs,” IEEE Transactions on Smart Grid, Vol. 5, No: 4, July 2014, pp.1808 -- 1814.

Göl, M. and Abur, A., “A Robust PMU Based Three-Phase State Estimator Using Modal Decoupling,” IEEE Transactions on Power Systems, Nov. 2014, Vol. 29, No: 5, pp.2292-2299.

Göl, M. and Abur, A., “Observability Analysis of Systems Containing Phasor Measurements,” Proceedings of the IEEE Power and Energy Society General Meeting, 22-26 July 2012.

Göl, M. and Abur, A., “Effective Measurement Design for Cyber Security,” Proceedings of the 18th Power Systems Computation Conference, August 18-22, 2014, Wroclaw, Poland.

Göl, M. and Abur, A., “PMU Placement for Robust State Estimation,” Proceedings of the North American Power Symposium, Sep. 22-24, 2013, Manhattan, KS.

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Acknowledgements

• National Science Foundation• NSF/PSERC• DOE/Entergy Smart Grid Initiative Grants• NSF/ERC CURENT

Jun Zhu, Ph.D. 2009

Jian Chen, Ph.D. 2008

Murat Gol , Ph.D. 2014

Former PhD Students:

Liuxi Zhang, Ph.D. 2014

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