Protection and Control Issues associated with Shunt ...

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University of Tennessee Knoxville, TN October 26, 2018 Protection and Control Issues associated with Shunt Compensated Transmission Lines Pratap G Mysore Pratap Consulting Services, LLC

Transcript of Protection and Control Issues associated with Shunt ...

Page 1: Protection and Control Issues associated with Shunt ...

University of Tennessee

Knoxville, TN

October 26, 2018

Protection and Control Issues

associated with Shunt Compensated

Transmission Lines

Pratap G Mysore

Pratap Consulting Services, LLC

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CAPX2020 Project

Joint Initiative of eleven transmission owning utilities in

four states in upper Midwest.

800 miles of transmission at 345 kV and 230 kV

Largest transmission project in 40 years to improve

reliability of the grid in upper Midwest.

Last line expected to be energized in December 2018.

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Acknowledgement

American Transmission Company (ATC) study group for

bringing up DCZ issues during the line design studies on one

of the CAPX lines.

Failures of Breakers tripping immediately following shunt

compensated Line energization in Arizona.

This prompted three utilities associated with CAPX to

investigate the impact of shunt reactors on their lines and to

determine mitigation methods.

Paul Nyombi of Xcel Energy and Derrick Schlangen of

Great River Energy for their support and contribution to this

presentation.

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Transmission Line Representation

Long Transmission lines can be represented as several series connected

modules made up of series resistance, series inductance and shunt

capacitance.

Lines are also represented with lumped parameters where the line capacitances

are split between two ends.

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Line Parameters – Typical

345 KV System

Line Resistance: 0.033 Ω/Mile

Line Reactance: 0.5-0.6 Ω/Mile

Line Inductance: 1.459 mH/Mile

Line Charging MVAR: 0.8-0.9 MVAR/Mile

Line Capacitance:0.0189 µF/mile

Resistance can be ignored for our discussions.

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Transmission Line voltages

During light load or no load conditions, Transmission line

has the same effect as capacitance connected to the system.

System voltage increases with the connection of open ended

or lightly loaded transmission line.

Capacitance of the line is distributed over the entire length.

Open ended line voltage increases with increase in length.

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Shunt Reactor Application

• To keep system voltage below allowable maximum value

• System voltage needs to be within the allowable range to

prevent connected equipment failures.

- IEEE 1312- 1993 (R2004) “IEEE Standard Preferred Voltage Ratings

for Alternating-Current Electrical Systems and Equipment Operating at

Voltages Above 230 kV Nominal”

• Installed on

–Tertiaries of transmission transformers

– On transmission lines –either at both ends or at only one end.

–Middle of the line.

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Shunt Compensated Lines

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Effect of Shunt Reactors

Decreases the voltage by compensating for the capacitive

charging currents.

Reactor current, IL lags voltage by 900

Capacitor (line charging) current, IC leads voltage by 900

Decreases the current through the breaker current (|IC |- |IL |)

(f ile Paper1.pl4; x-v ar t) factors:

offsets:

1

0

v :I_L1 1.00E-03

0

c:I_C2 - 1

0

c:I_L1 -I_L2 1

0

c:XX0002-I_L1 1

0

0 10 20 30 40 50 60 70*10 -3

-300

-200

-100

0

100

200

300

Steady State current and Voltage phase relationship9

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Line Currents During Energization

Voltage waveform: V Sin (ωt +φ) where φ is the delay angle

of switching on the voltage waveform from voltage zero.

Charging (capacitive) current: I Sin(ωt+φ+90)

Reactor current: MI [Sin (ωt+φ-90)+ Cosφ e-t/τ]

(f ile Paper1.pl4; x-v ar t) v :XX0006

0.00 0.02 0.04 0.06 0.08 0.10-300

-200

-100

0

100

200

300

*103

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Line Breaker Current

IC = I Cos(ωt+φ)

IL = MI[-Cos(ωt+φ)+ Cosφ e-t/τ]

Breaker Current, IBRφ= IL+IC

IBRφ= IL+IC =(1-M)I Cos(ωt+φ) + MI Cosφ e-t/τ

Maximum DC offset is seen when the line with reactor is

switched at voltage zero crossing.

IBR0 = (1-M)I Cos(ωt) + MI e-t/τ

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Line Breaker Current Components

AC sinusoidal wave has a peak value of (1-M)I

DC component has a value of MI and is exponentially

decaying with time constant of τ sec.

X/R of oil filled reactors are in the range of 600-750; τ can

be as high as 2 seconds (~=750/377).

DC component will decay to less than 2% of the initial value

after 4τ time.

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Line Breaker Delayed Current Zero

If AC component peak (1-M)I is greater than DC component

MI, AC waveform will always cross current zero axis or else,

current zero occurs after a delay.

If the DC peak MI is greater than (1-M)I, first current zero

appears after several cycles

Delayed

Current

Zero

-0.5

0

0.5

1

1.5

2

2.5

3

3.5Delayed Current Zero (DCZ)

DC Component

Breaker Current

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Criterion to Prevent DCZ during Normal Switching

Boundary Condition: (1-M)I = MI;

M = 0.5;

Under normal switching, the degree of compensation, M

should not exceed 50% to prevent Delayed Current Zero on

breaker current.

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Time to first Current Zero

0

0.2

0.4

0.6

0.8

1

1.2

0 2 4 6 8 10

Deg

ree

of

Co

mp

ensa

tio

n

Time for first current zero

Degree of Compensation VS Time to

first Current Zero (τ =2 sec)

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Effect of Inserting resistance in the circuit

The time constant of DC Component is the overall time constant

of the system: (Xtotal/Rtotal))

If breakers are equipped with pre-insertion resistors ( 250-400

ohms)

Overall X/R reduces. DC component decays faster.

ZReactor = 3.174 + j2380.49 (50 MVAR, X/R =750)

Zsystem = 2.491 + j47.5 (assuming 2500MVA , X/R= 17)

Without pre-insertion resistor, Ztotal = 5.665+j2428 (X/R=428)

Pre-insertion resistance = 400 ohms

Ztotal = 405.665 +j2428 (X/R= 6); Time constant: 16ms

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Energizing a Faulted line

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Mitigation Methods – Control and Protection

Considerations Energize a line without shunt reactor

Use a breaker capable of interrupting DC current – Single interrupter

SF6 design has very low DC interrupting capability

Use controlled closing – Has mechanical tolerance limitation

Use of resistance in the neutral of the reactor bank.

Use of pre-insertion resistor

Limit or reduce degree of compensation to less than 50% during line

energization or during reclosing

Switching issues associated with tripping the reactor during line

faults and also during re-energization onto the energized line.

Tripping issues for shunt reactor faults

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Simulation Results- Simplified System Model

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Delayed Current Zero Mitigation Methods

A. Use of pre-insertion resistors

a. With both shunt reactors

connected (approx. 86%

compensation)

b. With both shunt reactors

connected and utilization

of 425ohm pre-insertion

resistors inserted for 13ms

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.10 0.25 0.40 0.55 0.70 0.85 1.00-700

-525

-350

-175

0

175

350

525

700

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.190 0.252 0.314 0.376 0.438 0.500-200

-150

-100

-50

0

50

100

150

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Delayed Current Zero Mitigation Methods

B. Energizing the line with reduced degree of compensation

Line energization cases – Line breaker currents

a. With both shunt reactors

connected (approx. 86%

compensation)

b. With only north end

reactor connected

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.10 0.25 0.40 0.55 0.70 0.85 1.00-700

-525

-350

-175

0

175

350

525

700

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50-600

-400

-200

0

200

400

600

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Delayed Current Zero Mitigation Methods

C. Utilization of controlled switching of shunt reactors

and the impact of power flow on line breakers

South line end current following

energization of South line-end

shunt reactor on a closed through

transmission line with North line-

end reactor connected. Approx. 46

MW are flowing on the line

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.3 0.4 0.5 0.6 0.7 0.8-120

-80

-40

0

40

80

120

South Substation line breaker current

following uncontrolled closing of

South line-end reactor with limited

power flow on the line

(f ile North_South_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BB-STH_LB c:STH_BC-STH_LC

0.38 0.40 0.42 0.44 0.46 0.48 0.50 0.52-200

-150

-100

-50

0

50

100

150

200

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Reactor Energization Field Record

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Reactor Currents Line breaker CurrentsWith 74 MW load

(f ile CMD.pl4; x-v ar t) c:X0018A-X0032A

0.0 0.2 0.4 0.6 0.8 1.0-140

-105

-70

-35

0

35

70

105

140

(f ile CMD.pl4; x-v ar t) c:X0018A-X0032A

0.0 0.2 0.4 0.6 0.8 1.0-300

-200

-100

0

100

200

300

ATP Simulation -Line breaker

Current (A-Ph) with 74 MW

load

ATP Simulation -Line breaker

Current (A-Ph) with No load

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Other Delayed Current Zero Mitigation Methods

Consider moving some reactors (or some of them) from

transmission lines to substation buses

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Tripping and reclosing considerations for shunt

compensated lines

Reactor current following a

SLG fault:

A-Phase to ground fault is

considered to occur at A-Phase

voltage zero crossing.

Shunt reactor current takes

several cycles to decay to zero;

τ~ 1.68s

(f ile North_South_345kV.pl4; x-v ar t) c:STH_LA-STH_RA

0 2 4 6 8 10-120

-80

-40

0

40

80

120

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First, consider a SLG fault on the line

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Tripping and reclosing considerations for shunt

compensated lines

For faults on transmission lines, only the line breakers should be

tripped.

It’s recommended to disable high-speed reclosing. For lines with

more that 50% compensation, some shunt reactors may need to be

switched out, after the shunt reactor current decays to zero, before

re-energization of the line. However, this may take as long as

4*1.68 ~ 7 seconds.

Radial energization of the line, with reduced compensation is

suggested. Remote breaker may synch-close after a definite time

delay

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Tripping and reclosing considerations for shunt

compensated lines

Delaying line breaker tripping for transmission line faults is

suggested – allows for appearance of current zero crossing for

faults (during light load periods) on lines with more than 50%

compensation. South line-end currents are shown below for close-

in A-G fault

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(f ile North_South_345kV.pl4; x-v ar t) c:STH_BB-STH_LB c:STH_BC-STH_LC

0.35 0.39 0.43 0.47 0.51 0.55-300

-200

-100

0

100

200

300

400

500

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Tripping for shunt reactor faults

Trip only the shunt reactor for reactor faults and not the line

especially during shunt reactor switching onto the energized line

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(f ile BIS_ALS_345kV.pl4; x-v ar t) c:STH_BA-STH_LA c:STH_BC-STH_LC

0.0 0.1 0.2 0.3 0.4 0.5 0.6-300

-200

-100

0

100

200

(f ile BIS_ALS_345kV.pl4; x-v ar t) c:STH_LA-ALS_RA c:STH_LC-ALS_RC

0.0 0.1 0.2 0.3 0.4 0.5 0.6-300

-250

-200

-150

-100

-50

0

50

100

Line breaker currents on unfaulted phases Unfaulted phase reactor currents

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Conclusions

A. On line energization to prevent DCZ

If shunt reactor(s) on the line is not required to limit open end

voltage to acceptable level, energize the line without shunt

Reactors.

Keep shunt compensation below 50% during line

energization.

Energize the line through breakers equipped with pre-insertion

resistors that provide enough damping to produce current

zeros within breaker interrupting time. This is dependent on

the resistor value and duration of insertion. It may not work

under all the cases if the degree of compensation is close to

100%.

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Conclusions

B. On Shunt reactor energization onto energized lines, to

prevent DCZ

Switch shunt reactors less than 50% of the total charging

current.

Switch shunt reactor at voltage maximum point on the wave.

Switch shunt reactors if the minimum load on the line, in MW

exceeds reactor MVAR rating.

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Conclusions

C. Tripping for line faults

Trip only the line breakers and not shunt reactors.

Shunt reactors need to be tripped only after several seconds

delay to allow full decay of reactor current on the faulted

phase.

Total interrupting time of faults on lines with shunt

compensation greater than 50% may need to be at least few

cycles to allow presence of current zeros on healthy phase(s)

during faults. This is dependent on the zero sequence currents

flowing on the healthy phases or the minimum load on the

healthy phases.

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Conclusions

D. Tripping for shunt reactor faults

Trip only the shunt reactors

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Conclusions

E. Reclosing on Lines:

Instantaneous reclose is disabled on lines where shunt reactor

switching is required to reduce the degree of compensation.

Time delay reclose is enabled after the reactor is switched out.

Synch-check reclosing at the other end after energizing the

line may generate offsets on the currents. DC offset is

dependent on the load picked up after restoration.

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Research topics

•Mechanisms to interrupt DC

•Breakers with longer Pre-insertion times

•Controls to insert reactors immediately

following simultaneous closing of line

breakers at both ends.

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Questions

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