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1 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Superconducting Fault Current Limiters and Magnetic Leviation European Summer School on Superconductivity 2008 June 11-18, 2008 at Prizztech Magnet Technology Centre, Finland Prof. Dr.-Ing. Mathias Noe, Forschungszentrum Karlsruhe, Institute for Technical Physics

Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

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Page 1: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

1 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Superconducting Fault Current Limiters and Magnetic Leviation

European Summer School on Superconductivity 2008

June 11-18, 2008 at Prizztech Magnet Technology Centre, Finland

Prof. Dr.-Ing. Mathias Noe, Forschungszentrum Karlsruhe, Institute for Technical Physics

Page 2: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

2 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Outline

Superconducting Fault Current Limiters• Motivation and Basics of Fault Current Limitation• Different Types of SCFCLs• Application of SCFCLs• State-of-the-ArtMagnetic Levitation• Principle and Applications

Page 3: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

3 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

„it is impossible to avoid short-circuit currents“

Motivation

Page 4: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

4 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

22.6.2005 – Blackout in swiss train system

BlackoutDamage

Consequences of Short-Circuits

Page 5: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

5 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Simplified Electrical Circuit

Grid Transformer Transfer Line Load

Peak short-circuit current Kp Ii ′′≤ 22

j XQ j XT j XL

Stationary Electrical Circuit (Three phase short-circuit)

3nUc

RLRTRQ

LTQK ZZZZ ++=

kI ′′

k

b

n

K

n

nb

k

nk Z

ZcIIgetwe

IUZwith

ZUcI =

′′==′′

33

c=1.1 for high SC currents

c=1 for low SC currents

Page 6: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

6 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Conventional Measures to Limit Short-Circuit Currents

• Splitting into sub grids

• Introducing ahigher voltage range

• Splitting of bus bars

• (Sequential tripping)

• High impedancetransformers

• Current limitingair core reactors

Novel Concepts

• Superconductors

• Semiconductorse.g. FACTS

• Hybrid systems

Topologicalmeasures

Apparatusmeasures

PassiveIncrease of impedance at

nominal and fault conditions

ActiveSmall impedance at nominal loadfast increase of impedance at fault

• High voltage fuses(< 1 kA, < 36 kV)

• IS-limiter, CLiP(< 4 kA, < 36 kV)

• FCL circuit breakers

Page 7: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

7 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Outline

Superconducting Fault Current Limiters• Motivation and Basics of Fault Current Limitation• Different Types of SCFCLs• Application of SCFCLs• State-of-the-ArtMagnetic Levitation• Principle and Applications

Page 8: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

8 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

RSC

LQ Switch

RQ

U0

iac

Rp

SCFCL

Load

Different SCFCL TypesResistive SCFCL (pure resistive)

Electric circuit

Page 9: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

9 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Without limiter

Normal op. Short-circuit Recovery

Time

Cur

rent RSC=0

LQ

RQ

U0

iac

Rp

iac

Different SCFCL TypesResistive SCFCL (pure resistive)

Electric circuitOperation modes

Switch

SCFCL

Load

Page 10: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

10 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Normal op. Short-circuit Recovery

Time

Cur

rent

WithoutSCFCL

RSC>0

LQ

RQ

U0

iac

Rp

iac

Different SCFCL TypesResistive SCFCL (pure resistive)

Electric circuitOperation modes

Switch

SCFCL

Load

Page 11: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

11 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Normal op. Short-circuit Recovery

Time

Cur

rent

WithoutSCFCL

RSC→0

LQ

RQ

U0

iac

Rp

iac

Different SCFCL TypesResistive SCFCL (pure resistive)

Electric circuitOperation modes

Switch

SCFCL

Load

Page 12: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

12 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Normal op. Short-circuit Recovery

Time

Cur

rent

WithoutSCFCL

RSC→0

LQ

RQ

U0

iac

Rp

iac

+ compact, low weight+ fail safe- current leads to low temperatures

Characteristic

Electric circuitOperation modes

Different SCFCL TypesResistive SCFCL (pure resistive)

Switch

SCFCL

Load

Page 13: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

13 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

RSC

LQ S

RQ

U0

iac

ip Lp

iSCA

B

+ compact, low weight+ fail safe- current leads to low temperatures

SCFCL

Electric circuit

Characteristic

Different SCFCL TypesResistive SCFCL (resistive-inductive)

Page 14: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

14 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Electric circuit

iD

uD

I02

Diode characteristic

forward

reverse

LLQ

D1

D4

D3

D2

S

UbRQ

U0

iac

I0

SCFCL

Load

Different SCFCL TypesBridge Type SCFCL

Page 15: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

15 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

LLQ

D1

D4

D3

D2

S

UbRQ

U0

iac

I0

Normal operation, no limitationiac < I0 SCFCL

iD

uD

I02

forward

reverse

iac2

Load

Electric circuitDiode characteristic

Different SCFCL TypesBridge Type SCFCL

Page 16: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

16 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Short-circuit and limitationiac > I0

iD1,2

uD

I02

Positive half wave iacD1, D2 conduct

D3, D4 arrest if iac>I0

iD3,4

uD

I02

LLQ

D1

D4

D3

D2

S

UbRQ

U0

iac

I0

SCFCL

Load

Electric circuitDiode characteristic

Different SCFCL TypesBridge Type SCFCL

Page 17: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

17 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Short-circuit and limitationiac > I0

iD1,2

uD

I02

Negative half wave iacD1, D2 arrest if iac>I0

D3, D4 conduct

iD3,4

uD

I02

LLQ

D1

D4

D3

D2

S

UbRQ

U0

iac

I0

SCFCL

Load

Electric circuitDiode characteristic

Different SCFCL TypesBridge Type SCFCL

Page 18: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

18 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

LLQ

D1

D4

D3

D2

S

UbRQ

U0

iac

I0

SCFCL

iD

uD

I02

forward

reverse

Load

+ no superconductor quench (L can be non-SC)+ immediate recovery+ adjustable trigger current (depends on I0)- not fail safe- losses in semiconductors

Characteristic

Electric circuitDiode characteristic

Different SCFCL TypesBridge Type SCFCL

Page 19: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

19 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

C1

Laod

LQ

RQ

U0

SCFCL

iACvL1 vL2

H1B1

H1

11

1

dBLdH

=

H2B2

H22

22

dBLdH

=

Electric circuitIron core characteristic

Different SCFCL TypesDC biased Iron Core

Page 20: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

20 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

C1

Load

LQ

RQ

U0

SCFCL

iACvL1 vL2

iDC1 iDC2

H1B1

H1

11

1

dBLdH

=

H2B2

H22

22

dBLdH

=

HDC1

HDC2

Electric circuitIron core characteristic

Different SCFCL TypesDC biased Iron Core

Page 21: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

21 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

C1

Load

LQ

RQ

U0

SCFCL

iACvL1 vL2

iDC1 iDC2

H1B1

H1

11

1

dBLdH

=

iacU0

H2B2

H22

22

dBLdH

=

t

HDC1

HDC2

Electric circuitIron core characteristic

Different SCFCL TypesDC biased Iron Core

Page 22: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

22 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

C1

Load

LQ

RQ

U0

SCFCL

iACvL1 vL2

iDC1 iDC2

Characteristic

+ no superconductor quench, immediate recovery+ superconductor for DC only+ adjustable trigger current- high volume and weight- high impedance during normal operation

H1B1

H1

11

1

dBLdH

=

iacU0

( )

Δ = +

= +

1 2

1 2ac

v V VdiL Ldt

H2B2

H22

22

dBLdH

=

t

HDC1

HDC2

Electric circuitIron core characteristic

Different SCFCL TypesDC biased Iron Core

Page 23: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

23 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Different SCFCL Types

And many other superconducting types

• Shielded core type

• Fault current controller

• Hybrid

• Flux lock type

And many other non-superconducting types

• Solid state breaker

• Series line compensation

• Polymer PTC resistor

• Driven arc switch

• Array of liquid metal switches

• Hybrid switch arrangement

Page 24: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

24 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Outline

Superconducting Fault Current Limiters• Motivation and Basics of Fault Current Limitation• Different Types of SCFCLs• Application of SCFCLs• State-of-the-ArtMagnetic Levitation• Principle and Applications

Page 25: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

25 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Transmission network

SL-Kabel

Distribution network

Distribution network

Distributionnetwork

SCFCL Applications

Page 26: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

26 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Source:Noe, M.; Oswald, B.R., “Technical and economical benefits of superconducting fault current limiters in power systems”, IEEE Trans. Appl. Supercon. Vol. 9/2, June 1999, pp. 1347 –1350

Transmission network

1

2

3

11

FCL

6

7

8

5

9

10

4

SL-Kabel

FCL

FCL Distribution

networkDistribution

network

FCL FCL 9

FCL

FCL FCL

FCL FCL

FCL

FCL

Distributionnetwork

1 Generator feeder2 Power station auxiliaries3 Network coupling4,5 Busbar coupling6 Shunting current limiting reactor7 Transformer feeder8 Busbar connection9 Combination with other SC devices,especially SC cables10 Coupling local generating units11 Closing ring circuits

SCFCL Applications

Page 27: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

27 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Source:Fault Current LimitersReport on the Activities of CIGRE WG 13.10by CIGRE Working Group 13.10 (*), CIGRE Session 2004, Paris

• above

Feeder

Generator feederBusbar coupling

Transformer feeder

18%

15%

52%

15%

Which voltage level? Which location?

> 145 kVto 36 kV to 145 kV

87%

2%11%

SCFCL Applications

Page 28: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

28 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

110 kV

10 kV grid

GeneratorTransformer

G

5...50 MVA

10 kV SCFCL

Coupling of decentralized Power Generation with SCFCLs

Page 29: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

29 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

G

Transmissiongrid

MM

SCFCL

SCFCLSCFCL

SCFCLSCFCL

SCFCL

a) Medium voltage (e.g. 10 kV)b) Medium voltage (e.g. 10 kV)c) Low voltage (e.g. 0.4 kV)

a)

b)

c)

M

SCFCLs in Power Plant Auxiliaries

Page 30: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

30 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Substation B

CB

CB CB

CB

Substation A

Substation C

CBG1

NewGenerator

SCFCL

CB

CB CB

CB

SCFCL in Generator Feeder Location

Page 31: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

31 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

SCFCL

380 kV

220 kV

220 kV

380 kV

220 kV

380 kV

380 kV

110 kVB

110 kVA

Details: C. Neumann, SCENET Workshop on Superconducting Fault Current Limiters, Siegen, Germany, June 28-29 2004

Two Subgrids coupled with SCFCLs(e. g. RWE)

Weight: 383 tOil: 70 t

18 m

10 m

Page 32: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

32 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

CB6 CB3

CB8

Load flow

S1

S3

S2

SCFCL

CB2

G1

CB5

CB1

CB4

CB9 CB11 CB10

CB7

CB14 CB15 CB12

CB13 G2

154 kV GISsubstation

in Seoul

High Voltage Busbar Coupling

Page 33: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

33 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Outline

Superconducting Fault Current Limiters• Motivation and Basics of Fault Current Limitation• Different Types of SCFCLs• Application of SCFCLs• State-of-the-ArtMagnetic Levitation• Principle and Applications

Page 34: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

34 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Important FCL projectsImportant FCL projects

- State-of-the-art -

Lead company Country / Year Type Data SC type

KfK Germany / 1980 Resistive 40 MW / 47 kV NbTi

GEC Alsthom France / 1989 Resistive 25 kV / 200 A NbTi

GEC Alsthom France / 1992 Resistive 7.2 kV / 1 kA NbTi

GEC Alsthom France / 1994 Resistive 63 kV / 1.25 kA NbTi

NEI UK 1979 Sat. iron core 5 MVA NbTi

ASC / General Dynamics US / 1995 Sat. iron core 100 MVA BSCCO

ABB Switzerland / 1989 Shielded iron core 100 VA BSCCO

ABB Switzerland / 1989 Shielded iron core 20 kVA BSCCO

Daimler Benz Germany / 1993 Shielded iron core - YBCO

Hydro Quebec Canada / 1993 Inductive 100 VA BSCCO

Hydro Quebec Canada / 1995 Inductive 100 kVA BSCCO

TEPCO / Toshiba Japan / 1990 Inductive air coil 400 V / 100 A NbTi

Sekei Uni. Japan / 1990 Inductive 600 V / 6 A NbTi

TEPCO / Toshiba Japan / 1990 Inductive air coil 6.6 kV / 1.5 kA NbTi

Actual and planned SCFCL projects in 1994

Page 35: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

35 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

FAULT CURRENT LIMITERSAmerican Superconductor - (DOE cost share: $12.7 million)American Superconductor will also address the development and in-grid testing of a three-phase high-voltage, 115-kilovolt fault current limiter, called a SuperLimiterTM, by using second-generation wire. The SuperLimiterTM features a proprietary Siemens-developed, low-inductance coil technology thatmakes the fault current limiter invisible to the grid until it switches to a resistive state. The demonstration will occur at a location operated by teammember Southern California Edison. The team also includes: Nexans (France), the University of Houston (Houston, TX), Los Alamos National Laboratory (Los Alamos, NM), and Siemens AG (Germany).

SC Power Systems - (DOE cost share: $11 million)On the Southern California Edison grid, SC Power Systems (San Mateo, CA) will design, test, and demonstrate a 138-kilovolt saturable reactor-type fault current limiter. In this type of fault current limiter, a high-temperature superconductor is used with a direct current power supply to saturate an iron corethat interfaces with the line in which the current is to be limited. SC Power’s team includes: DOE’s Los Alamos National Laboratory (Los Alamos, NM); Air Products and Chemicals Inc. (Allentown, PA); Cryo-Industries of America Inc. (Manchester, NH); Consolidated Edison Company (New York, NY); California Edison Inc. (Rosemead, CA); Delta Star Inc. (San Carlos, CA); and Trithor GmbH (Germany).

SuperPower Inc. - (DOE cost share: $5.8 million)SuperPower Inc. (Schenectady, NY) will design, test, and demonstrate on the American Electric Power grid a 138-kilovolt fault current limiter thatfeatures a matrix design consisting of parallel “second-generation” high-temperature superconductor elements and conventional coils. SuperPower’steam includes: Sumitomo Electric Industries Ltd. (Osaka, Japan); Nissan Electric Co. Ltd. (Kyoto, Japan); The BOC Group Inc. (Murray Hill, NJ); American Electric Power (Gahanna, OH); and DOE’s Oak Ridge National Laboratory (Oak Ridge, TN).

June 27, 2007

DOE Provides up to $51.8 Million to Modernize the U.S. Electric Grid SystemSuperconductor Research Crucial to Improving Power Delivery Equipment

Page 36: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

36 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

YBCO coated cond.

MgB2

YBCO coated cond.

YBCO coated cond.

BSCCO 2223 tape

BSCCO 2223 tape

YBCO coated cond.

YBCO coated cond.

YBCO coated cond.

BSCCO 2223 tape

BSCCO 2212 bulk

BSCCO 2223

BSCCO 2223 tape

BSCCO 2223 tape

YBCO thin films

YBCO thin films

YBCO thin films

BSCCO 2212 bulk

Superconductor

-6.6 kV, 400 A, -Resistive-Rolls Royce

+7.6 kV, 1.2 kA, 3-ph.DC biased iron core2008Zenergy Power

+66 kV, -, 3-ph.Resistive2011AMSC / Siemens

+80 kV, -, 3-ph.DC biased iron core2010Zenergy Power

-3,2 kV, 215 A, 3-ph.Resistive2005CESI Research

-3.8 kV, 200 A, 3-ph.Diode bridge2004Yonsei University

+6 kV, 1.5 kA, 3-ph.Diode bridge2005CAS

-3.8 kV, 200 A, 3-ph.Resistive2004KEPRI

-1 kV, 40 A, 1-ph.Resistive2004CRIEPI

-200 V, 1 kA, 1-ph.Resistive2004Mitsubishi

+6.6 kV, -, 3-ph.Resistive2008Toshiba

+22.9 kV, 3 kA, 3-ph.Resistive2010KEPRI

+80 kV, -, 3-ph.Resistive2009IGC Superpower

-13.2 kV, 630 A, 1-ph.Resistive2007Hyundai / AMSC

-7.5 V, 267 A, 1-ph.Resistive2007Siemens / AMSC

?20 kV, 1.6 kA, 3ph.DC biased iron core2007Innopower

-13.2 kV, 630 A, 3-ph.Res.-hybrid2007KEPRI

+6.9 kV, 600 A, 3-ph.Resistive2004ACCEL/Nexans SC

Field testData 2)TypeYear/Coutry 1)Lead company

1) Year of test2) Phase to ground voltage

Status of SCFCL development

Page 37: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

37 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Courtesy: Nexans SuperConductors

Rated voltage 12 kV

Rated current 800 A

Max. current 1.8 kA

Lim. time 120 ms

Lim. current < 27 kA

3-phase arrangement

Courtesy: Nexans SuperConductors

Bi 2212 component

Cou

rtes

y:

Nex

ans

Supe

rCon

duct

ors

First Commercial SCFCL Installation

Page 38: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

38 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Objective

• Development and in-grid testing of a 3-phase high voltage 115 kV, 1.2 kA SCFCL

• Funded by US DOE; partners AMSC, Siemens, Nexans, LANL; budget $ 25.4 million for4.5 years (2007-2012)

Benefit

• Enable load growth and higher reliability in grid networks

Siemens

• Grid integration studies

• Development of switching module (coil stack)

• Design of HV and cryogenic system

• Laboratory pre-tests

Nexans

• Current leads

Resistive Type SCFCLAMSC/Siemens

Page 39: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

39 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Resistive Type SCFCLSuperpower

Test arrangementCurrent and voltage

Objective: 138 kV SCFCL until 2009

Page 40: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

40 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Courtesy: Zenergy Power Short-circuit tests at Powertech Labs British

Columbia, December 2007

Bi 2223 DC coil

13 kV, 1.2 kA

DC biased Iron Core

Page 41: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

41 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Diode Bridge Type SCFCL in China 10 kV, 1.5 kA

First successful field test of a diode bridge type SCFCL at Gaoxi substation in Hunan / China since October 2005

Installation at Gaoxi substation

HTS coil

DataVoltage 10.5 kVLightning voltage 75 kVCurrent 1.5 kACoil inductance 6.24 mH

LLQD1

D4

D3

D2

S

RQ

U0

iac

SCFCL

Load

IGCT

Page 42: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

42 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Obejctive (99’-2005)Development and field test of a 10 kV, 10 MVA SCFCL demonstrator

DataVoltage 10 kVCurrent 600 Power (3 ph.) 10 MVAShort-circuit time 60 msMax. short-circuit current 8.75 kA (5 ms)

PartnerACCEL Coordination, System engineeringRWE Energy Field test, Specification E.ON SpecificationNexans SuperConductors MCP-BSCCO 2212 developmentATZ YBCO developmentEUS power system simulationACCESS FEM simulationForschungszentrum Karlsruhe Material characterization and quench tests

BMBF Project CURL10

Page 43: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

43 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

BMBF Project CURL10

Page 44: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

44 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Setup:

Data:Outer diameter: 58 mmSuperconductor length: 5.4 mSupercondcutor cross section: 0.24 cm²Critical current (65K): 850 APower (65K): >130 kVA

Data:Outer diameter: 58 mmSuperconductor length: 5.4 mSupercondcutor cross section: 0.24 cm²Critical current (65K): 850 APower (65K): >130 kVA

Most powerful element for resistive SCFCLs !Most powerful element for resistive SCFCLs !

StabilisationBSCCO 2212

Shunt

Isolation

Solder

BMBF Project CURL10MCP-BSCCO2212 bifilar coils (Nexans SuperConductors)

Page 45: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

45 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

CURL10 field test in Netphen April 2004-March 2005

BMBF Project CURL10

SCFCL

110 kV15 MVA

uk = 12,5 %Sk = 125 MVA

Load

10 kV

Page 46: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

46 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

60 70 80 90 100 110 120-8

-6

-4

-2

0

2

4

6

810 kV, 65 K, FGH

Phase 1 Phase 2 Phase 3

Cur

rent

/ kA

Time / ms60 70 80 90 100 110 120

-18-16-14-12-10-8-6-4-202468

1012

10 kV, 65 K, FGH Phase 1 Phase 2 Phase 3

Volta

ge /

kV

Time / ms

Final three phase short-circuit test of CURL10 (October 2003)

BMBF Project CURL10

Page 47: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

47 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

BMBF Project CURL10

Page 48: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

48 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

FCLG

High current feeder with generator, SCFCL and cable+ compact very high current connection+ high normal current, low short-circuit current

FCL

Fault current limiting cable+ active current limitation+ lower short-circuit rating

FCL

Fault current limiting transformer+ active current limitation+ less volume, less weight, oil free

Current Limiting Systems

Page 49: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

49 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

• Low loss, high current conductors

• Simple and inexpensive SCFCLs for medium voltage application(R&D of prototypes and pre-commercial units for field tests)

• SCFCLs for high voltage applications >100 kV(R&D of first demonstrators)

• Work on standards(e.g. tests, specification, requirements, CIGRE WG A13.16)

Future R&D on SCFCLs

Page 50: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

50 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Outline

Superconducting Fault Current Limiters• Motivation and Basics of Fault Current Limitation• Different Types of SCFCLs• Application of SCFCLs• State-of-the-ArtMagnetic Levitation• Principle and Applications

Page 51: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

51 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

vS

IS

BP

FZ

FX

IP

BS

Principle Magnetic forces

Electrodynamic Levitation

Page 52: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

52 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

vS

IS

BP

FZ

FX

IP

BS

Principle Track

Electrodynamic Levitation

Page 53: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

53 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

vS

IS

BP

FZ

FX

IP

BS

Principle Yamanashi Test Line (Japan)

Opening 1996Length 42.8 km581 km/h in 2003

Source: Railway Technical Research Institute

Electrodynamic Levitation

Page 54: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

54 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Courtesy: IFW Dresden

PrincipleSuper-

conductor

Permanent magnets

Small toy

Absolute contactless transportation system• Contactless levitation and guidance system• Contactless propulsion• Contactless control- and positioning system• Contactless energy transmission to the vehicle

Electromagnetic Levitation with Superconductors

Page 55: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

55 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

PrincipleSuper-

conductor

Permanent magnets

Demonstration Supratrans

Courtesy: IFW Dresden

Absolute contactless transportation system• Contactless levitation and guidance system• Contactless propulsion• Contactless control- and positioning system• Contactless energy transmission to the vehicle

Electromagnetic Levitation with Superconductors

Page 56: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

56 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

HTC

Rotating shaft

CryostatCopper

Permanent magnet Iron

Superconducting Bearings

Page 57: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

57 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

10 kN HTS Bearing (Siemens/Nexans/TU Braunschweig)

270 YBCO single crystall40x40x14 mm³

Cryostat with coldhead Bearing completeHTS and copper

Rotor NdFeBpermanent magnets

n: 3600 1/min

Top: ≤ 65 K

Weight: 10 kN

Page 58: Superconducting Fault Current Limiters and … | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation Outline Superconducting Fault

58 | Mathias Noe | European Summer School – Superconducting Fault Current Limiters and Magnetic Leviation

Prof. Dr.-Ing. Mathias NoeForschungszentrum KarlsruheDirector Institute for Technical PhysicsHermann-von-Helmholtz-Platz 176344 Eggenstein-LeopoldshafenGermany

Phone: ++49 +7247 82 3500Fax: ++49 +7247 82 2849Email: [email protected]

Mathias Noe has received his M.S. in Power Engineering in 1991 and his Ph.D. (thesis on “SCFCLsas new devices in power systems”) in 1998, both from the University of Hanover in Germany. After a Postdocposition at the Ecole Polytechnic Federale de Lausanne in Switzerland, he joined Forschungszentrum Karlsruhe in 1998 and became later group leader for HTS power devices at the Institute for Technical Physics.Since 2006 he is director of the Institute for Technical Physics at the Forschungszentrum Karlsruhe and full professor for technical applications of high temperature superconductivity at the faculty of electrical engineering and information technology of the University Karlsruhe. He is board member of the European Society of Applied Superconductivity, board member of the Magnet Technology conference, secretary of the CIGRE working group WG D.15 “Superconducting and insulating materials for HTS power applications”. Prof. Noe is a registered member of the VDE, the German society of electrical engineers.

Biography