1018498_combined
TRANSCRIPT
Task Force on Fault Current Limiter Testing
Frank C. LambertGeorgia Tech - NEETRAC
&
Michael „Mischa“ SteurerCenter for Advanced Power Systems,
Florida State University, Tallahassee, FL
Presented at the 8th EPRI Superconductivity Conference Oak Ridge, TN, Nov 12, 2008
11/12/2008 FCL_Testing_TF_EPRI-SC_Lambert_Steurer_12nov2008 2
New IEEE Task Force
• Goal– Develop a guide for testing novel FCL technologies (SC and
non-SC)– Complements activities by CIGRE WG-A3.23
• Scope– Identify FCL testing requirements from a utility point of view– Identify specific testing needs regarding the different FCL
technologies (e.g. superconducting vs. power electronics)– Identify applicability of existing power equipment testing
standards– Recommend additional tests and testing procedures as needed– Identify gaps in availability of testing capabilities and recommend
power requirements for upgrading
11/12/2008 FCL_Testing_TF_EPRI-SC_Lambert_Steurer_12nov2008 3
New IEEE Task Force
• Approach– Study and review novel fault current limiter (FCL) technologies
for medium and high voltage systems.– Map testing requirements against the needs by different FCL
technologies– Map testing requirements against existing power equipment
testing standards– Map testing requirements against available laboratory
capabilities– Coordinate with other technical committees, groups, societies
and associations as required• Status
– New IEEE task force was approved by the IEEE Switchgear Committee in October 2008
– We still need participants!• First meeting possible during the Joint Technical Committee
Meetings in Atlanta (http://www.pestechnical.com) January 12 – 15, 2009
• Next regular meeting of the IEEE Switchgear Committee will be in Asheville, NC, May 3 – 7, 2009
11/12/2008 FCL_Testing_TF_EPRI-SC_Lambert_Steurer_12nov2008 4
NEETRAC Fault Current Limiter Needs Assessment Survey
• Goal– Help target and direct FCL development towards applications
with the maximum potential benefit for utilities• Approach
– NETRAC customer sponsored 10-page survey• Planning, Substation Engineering/Design• Operations/Maintenance• Protection & Control
– Individual utility responses will be collected and aggregated byNEETRAC
– Only composite results will be distributed to sponsoring NEETRAC members, survey participants, and CIGRE WG A3.23
• Status– Revisions of the survey questions are possible until mid of
January 2009– Interested parties please contact Frank Lambert
Email [email protected] 404-675-1855Fax 404-675-1820
Eighth Annual Superconductivity ConferenceCigre WG A3.23 Update
Ashok SundaramSenior Project Manager
(650) 855-2304
November 12th-13th, 2008Doubletree, OakRidge, TNHosted by DOE and ORNL
2© 2008 Electric Power Research Institute, Inc. All rights reserved.
“New” Cigre WG A3.23 on Application and feasibility of fault current limiters in power systems
• Met in Erlangen, Germany (near Nuremberg) hosted by Mr. Heino Schmitt of Siemens on Sept 3rd & 4th , 2008
• Twenty members selected worldwide to serve on this WG picked on a competitive basis from a large number of applicants
• Scope of the WG A3.23 is as follows:– Build on WG A3.10 and A3.16 and draw to a close A3’s
investigation into FCL’s– Location of FCL installation– Different type of FCL’s– Experience from former and new pilot projects– Feasibility of application of conventional and novel FCL’s– Acceptance issues and how to overcome them– Customer system requirements (fault level, insulation
coordination, power quality and stability)– Interactions with protection and other control and power devices– Potential economical savings (examples from utility experiences)
3© 2008 Electric Power Research Institute, Inc. All rights reserved.
“New” Cigre WG A3.23 on Application and feasibility of fault current limiters in power systems
• Time Schedule – 3 years
• Deliverables:– Technical brochure and report in Electra– Sessions symposium papers as appropriate– Tutorial material (enhancing that available from previous WG’s)
• Next Meeting– Early March 2009 sponsored by Zenergy (formerly SCPower) in
South San Francisco for a 2 days followed by a field visit to SCE to observe testing of Zenergy Superconducting FCL at the “Avanti” circuit of the future.
– Non members of the WG are welcome to attend and provide input but cannot participate in voting on motions passed.
4© 2008 Electric Power Research Institute, Inc. All rights reserved.
Reports from Cigre on Fault Current Limiters
• Cigre Technical Brochure No 239 (WG A3.10) December 2003.– Fault current limiters in electrical medium and high
voltage systems
• Cigre Technical Brochure No 339 (WG A3.16) February 2008– Guideline on the impacts of fault current limiting
devices on protection systems
5© 2008 Electric Power Research Institute, Inc. All rights reserved.
HTS CablesStatus of Standards Work
David LindsaySouthwire Company
EPRI HTS ConferenceOak Ridge, TN
12 Nov 2008
IEEE (www.ieee.org)
IEEEPES – Power & Energy Society
ICC – Insulated Conductor CommitteeC22D
C22D – Superconducting CablesInactive past ~5 yearsRe-activated in Oct 2008Discussion Group = no formal task for standard development at this time.Chair = David Lindsay
Cigre (www.cigre.org)
Cigre – International Council on Large Electric Systems
Study Committee B1 – Insulated CablesTF B1.31 – Testing of Superconducting Cable Systems
Created August 20081 year durationProvide terms of reference of future WGConvenor = David Lindsay
Cigre guides for HV/EHV cable are typically used as base for new IEC standards.
Proposal for US Sub-Committee on
HTS StandardsFrom Lance Cooley
IEEE-CSC Standards ChairAnd Bill Hassenzahl
Past IEEE-CSC Standards Chair
IEEE-CSC Standards• IEEE Council on Superconductivity recognizes
and supports standards activities– Hosted discussions 2004-2007 that led to new IEC-
TC90 working group on HTS current leads– Acts as liaison between individuals, organizations
(EPRI, IEEE, NEMA, Labs, Companies), and countries (IEC, VAMAS, CIGRE)
– Request to IEEE-CSC from Japanese National Committee for US participation in further work
• Proposal: IEEE-CSC will continue support as a liaison until a more formal organization is formed and funding can be secured
JNC-IEC Proposal• At the Berlin IEC TC-90 meeting the JNC proposed the creation of
an ad hoc group to discuss the validity of the general requirements of HTS (document available). The result of voting was 3 agreements(Japan, Korea and Poland) and 2 abstention (Germany and China). So the ad hoc group became possible to start. Professor Osamura was nominated as the Rapporteur. His comments to LD Cooley of the IEEE-CSC were:
• 1) The group should be organized by the experts from USA, Germany, Poland, China, Korea Japan and possibly others.
• 2) I feel this is very tough job for getting any reasonable conclusion whether its creation is valid or not.
• 3) So I would like to collect comprehensively opinions from the experts and also from people relating to SC science and technology. Please give me your opinion on this matter. And I would like to ask you to recommend the experts from USA.
• Cooley replied that we need to have general discussions in the USA and that we would provide a formal response in December 2008.
New IEC Ad-Hoc Group
October 9, 2008 Secretary IEC/TC90
Ad-hoc Group – 3: Standardization of Superconducting Wires Task: To study standardization issues on Superconducting wires and to report a result at the next TC90 meeting Member e-mail address Kozo Osamura (Japan) - Rapporteur
Koichi Nakao (Japan) [email protected] Jeonwook CHO (Korea) [email protected] Jacek Sosnowski (Poland) [email protected] TBD (USA) TBD (China)
Cooley (as of 11/7/08)
Motivation
• Groundwork by EPRI, IEEE-CSC, AEA DOE and others is working towards defining an effective organization
• Activity in, and request from, Japan requires a response at some level
• HTS conductors are becoming defined; end uses are developing; products are not yet there --- ripe for groundwork.
Potential US Committee Members approached by Cooley
• DOE: Haught• IEEE-CSC: Cooley, ‘Levy’• EPRI: Eckroad• NIST: Goodrich• NEMA: Liebowitz• AFRL: Barnes• NRL: Gubser
• NHMFL: Larbalestier• ORNL: Lee• LANL: Marken• GE: Bray• AmSC: Maguire, Fleshler• SuPwr: Xie, Martchevskii• AEA: Hassenzahl
Action items for coming year• Hold a workshop• Define an organizational structure• Prepare a Formal US response to JNC-IEC• Seek support• Assess landscape and needs
– Current leads already in progress– “WG1” – begin work on terminology– “WG2” – some characterizations need standards– Activities by CIGRE, EPRI, NEMA…
USA Formal Response to JNC• Details TBD• Suggest forming an ad hoc committee (following the IEC
plan) within the US with some or all of the individuals listed above.
• Suggest that the chair be from the IEEE-CSC and that this organization act as a coordinator for activities.
• During a workshop early in 2009 determine areas where standards are needed, both now and in the future.
• Address national and international issues in the standards area and how to establish a level playing field.
An Assessment of Fault Current Limiter Testing Requirements
Brian Marchionini &Ndeye K. Fall Energetics Incorporated
Dr. Michael “Mischa” Steurer Florida State University
EPRI Superconductivity Conference, November 12-13, 2008
What is a FCL and How Does it Work?
Fault
Very Low Impedance
Project Purpose and Scope
• Identify testing requirements for advanced electricity-delivery devices such as fault current limiters
• Make an assessment of the existing capabilities of testing facilities in the U.S. and internationally
• Perform a gap analysis to determine where existing testing capabilities and facilities fall short
• The scope of the project includes solid-state and superconducting-based fault current limiters
• Focuses on projects sponsored by the U.S. Department of Energy
Methodology
Testing NeedsTesting NeedsTesting Facility
CapabilitiesTesting Facility
Capabilities
Gap AnalysisGap Analysis
Subject Matter Expert InterviewsSubject Matter Expert Interviews
Organizations Contacted
Electrivation
Types of Testing
Specialized tests designed to obtain specific information.
Field tests during the lifetime of a system to detect deterioration.
IEC definition – “A test made before supplying of a general commercial basis of a system in order to satisfactory long term performance of the complete system.”
Verify that the device meets specifications before leaving the factory.
Tests performed to detect shipping or installation damage. Also reveals defects in workmanship.
Performed to demonstrate the adequacy of designs and materials of a system. Generally required when there is a significant change inmaterials or the manufacturing process.
Electrical and mechanical tests performed in a laboratory and conducted during development.
Description
Special-Purpose Tests
Maintenance Tests
Long-Term Prequalification Tests
Factory Production Tests
xCommissioning Tests
xType Tests
xResearch and Development Tests
Immediately needed
Category
Based on Table 3-2, on test categories for underground cable in EPRI Specifying and Testing HTS Power Equipment (Report number TBD)
Specifications for DOE’s FCL Projects
TransformerTransformer, Reactor, and Circuit Breaker
Transformer, Reactor, and Circuit Breaker
Cable, TransformerTesting Protocol Basis
20% to 40% reduction of a 60 kA to 80 kA fault
20%–50% reduction
50% reduction of an 80 kA fault
20–50% Reduction – 37 % at SCE (63 kA to 40 kA)
Fault Current Reduction
138 kV; 2,000 to 4,000 Amps steady-state; 3-phase
138 kV; 1200 Amps; 3-phase
69 kV; 3,000 Amps; 3-phase
138 kV, 2000 A Class (115 kV, 1200 Amps at SCE site); 3-phase
Ratings (final design)
• DC-based iron core• One DC first-generation HTS coil for a three-phase AC FCL• Saturable reactor-type FCL• Suitable for 2G materials, when available
• Resistive FCL• Matrix design has parallel, 2G HTS elements and conventional coils
Uses high power semiconductors Super-gate turn-off thyristor (SGTO)
• Resistive FCL• 3-phase, transmission voltage• Low-inductance bifilar coil switching module technology using 2G wire
Design
Zenergy PowerSuperPowerSilicon PowerAMSCSpecification
Current Status and Future Requirements of FCLs
0.1 1 100.1
1
10
100
Resistive HTSSaturated Iron CoreSolid State
Rated Current / kA rms
Line
-Lin
e V
olta
ge /
kV rm
s
AMSC
AMSC
Silicon Power
Zenergy
Silicon Power
Zenergy
SuperPower
SuperPower
Transmission
Distribution
Full Scale
Current Status
Examples of Test Facility Capabilities
Variable frequency and voltage converter
6.2 @ 4.161.5 @ 0.48
N/A4.160.481.15 (DC)
1.7134.8 (DC)
60 Hz power system grid fed from 12.47 kV
7.5 @ 4.161.5 @ 0.48
1300.3850.484.16
84137
0.140.140.1Tallahassee, FL
Florida State University-CAPS
2.2 MV, 220 kJ Impulse generator1MV Cascade Transformer
N/AN/A.1225 for 2 s1.002.201.00Atlanta, GANEETRAC
Short-circuit generator rated 4800 MVA at 18 kV
1000 MVA at 18 kV
4800 MVA24, 48, 72, 96 kV
154 kA @ 50/60 Hz at 18 kV
400 kV, 10 mA
4200 kV, 50 µs
400 kVChangwon, Korea
KERI
13.4-kV power grid; 1400 MVA generator
5 @ 13.4400 for 1 s
14004 (100 for ~1 sec. with upgrade)
0.025N/A0.138 (with upgrade)
Los Alamos, NM
LANL
DC and AC power suppliesN/AN/A0.3 (0.6 with upgrade)
500.30.8 0.2Oak Ridge, TN
ORNL
Power system grid (12,000 MVA)N/A150013.6110 for 3 s.1.003.000.80Vancouver, Canada
Power Tech
4 short-circuit generators, 2,100 MVA each
N/A840015 @50Hz17@60Hz
390 for 0.42 s.
1.002.601.00Arnhem, The Netherlands
KEMA
Short-circuit generators rated for 1,000 and 2,250 MVAparallel operation possible
N/A3250 13.850 for 1 s63 for 0.5 s.
0.100.800.55Chalfont, PAKEMA
Continuous Power
(MVA) @ nominal
voltage (kV)
Maximum (Surge) Power Rating (MVA)
No-load voltage (kV)
FaultDCLightning Impulse1/2/50μs
AC 50/60 Hz
Kind of Source(s) for the LabHigh-Power TestCurrent Test (kA) at “zero” voltage
Insulation Test (MV) at “zero”current
LocationName
Limited Current (kA)
Vol
tage
acr
oss
FCL
(kV
)
0
20
40
60
80
0 10 20 30 40 50 60 70 80 90 100
Testing Facility Gaps
SuperPower 90kA Prospective Fault with 50% reductionSuperPower 90kA Prospective Fault with 25% reduction
Source Capacity KEMA Holland
Source Capacity KEMA PASource Capacity PowerTech
Silicon Power 80 kA Prospective Fault with 25% reductionSilicon Power 80 kA Prospective Fault with 50% reduction
Zenergy 80 kA Prospective Fault with 50% reductionZenergy 80 kA Prospective Fault with 25% reduction
Source Capacity KEMA Holland with Ideal 4x Transformer
Major Findings – Part 1• T&D equipment testing facilities can provide voltage and
current to adequately test FCLs at the distribution level• There is no place that has the capabilities to test FCLs at
transmission-level current and voltage levels simultaneously
• While there is a need to conduct high voltage-current tests, “synthetic tests”, similar to the one’s used for circuit breakers, may be sufficient for certain tests
• There are a number of experts who believe advanced modeling and simulation may possibly substitute for certain tests
Zenergy’s FCL Device
Major Findings – Part 2• Commercial testing facilities are not always conducive for
advanced design and prototype testing for R&D projects
• Commercial T&D equipment testing facilities tend to be costly, busy, and difficult to schedule
• There are approximately 100 testing facilities around the world and these are equipped and managed to conduct routine tests of existing or market-ready devices to meet known standards and protocols
AMSC’s FCL module testing
Major Findings – Part 3• Today there are no common guidelines for testing
prototype high-temperature superconducting (HTS) and solid-state FCLs and for integrating these devices with the electric system
• Testing procedures have been and will continue to be developed by FCL device manufacturers and their utility R&D partners and will vary depending on the design of the equipment and the application
• This lack of standards complicates the testing process as each trip to the testing facility has unique requirements, protocols, and procedures
• The existence of standards could help expedite and accelerate the testing process
Conclusions• There is a need for testing facilities that have the flexibility
to respond to the special requirements of R&D projects• Given the unique capabilities of fault current limiters there
is an expectation that utilities will allow prototype FCLs to be installed and tested on their own systems, before they have been simultaneously tested for high current and high voltage
• There is a need to continue the discussionon FCL testing recommendations
SuperPower’s FCL module testing
Calculating required voltage
• System impedance w/o FCL (Ω1)= Single phase voltage/Fault current
• Required FCL impedance (Ω2)= Single phase voltage/Limited fault current
• Required voltage drop = (Ω1-Ω2) X Reduced fault current
Ashok SundaramEPRI
[email protected](650) 855-2304
Development of Test Protocol for 15kV Class Solid-State
Fault Current Limiter
Mahesh GandhiSilicon Power [email protected](484) 913-1520
2
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
9:30AM – 10:00AM
• SSCL Program Overview Ashok Sundaram
• SSCL Test Protocol Mahesh Gandhi
– SSCL design
– SSCL field test circuits
– SSCL test protocol
• Performance Verification testing at KEMA
• Pre-connection test (dielectric, partial discharge, etc.)
• Field operations testing (Steady-state test & Transient performance)
3
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
DSTATCOM
ENERGYSTORAGE
SOLID-STATEBREAKER
SSCL
DVR
ENERGYSTORAGE
SSTS
DYNAMICNON-LINEAR
LOAD
SENSITIVELOAD
CRITICALLOAD
UNINTERRUPTEDSUPPLY
REDUCEDSAGS, TRANSIENTS,
HARMONICS
SENSITIVE LOAD
COMPENSATEDVOLTAGE, POWER FACTOR
HARMONICS,
EPRI’s Smart Grid Power-electronic based Technologies
IUT RESIDENTIALLOAD
4
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Fault Current Management
• Growth in the generation of electrical energy and an increased
interconnection of the networks and distributed generation leads to
higher fault currents
• Higher fault causes more stress on the system reducing the life of
critical components such as transformers and has adverse impacts
on grounding.
• The growth in capacity requires replacing existing circuit breakers
with higher fault current ratings. Major cost impact and down time.
5
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Pat Duggan - ConEdison
“Fault Current Limiting functionality is a critical enabler for ‘open
access’ for new transmission and generation, and more cost effective
infrastructure upgrades and replacements. In addition fault current
limiters can mitigate recovery time of superconducting cables and
give selected DGs an advanced option to serve peak loads after
external faults.”
6
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
FCL Technology Taxonomy
• Splitting into sub grids
• Introducing a higher voltage range
• Splitting of bus bars
• High impedance transformers
• Current limiting reactors
novel concepts
• Superconductors
• Semiconductors
• Hybrid systems
Topologicalmeasures
Apparatusmeasures
Permanent impedance increaseduring nominal and fault conditions
Condition based impedance increaseSmall impedance at nominal loadfast increase of impedance at fault
• Fuse based devices(< 36 kV)
• Stand alone HV fuse(< 1 kA)
• Commutating Current Limiters (< 5 kA)
• Sequentialtripping
Old term:“passive” Old term:
“active”
Apparatusmeasures
Topologicalmeasures
New terminology as defined in previous EPRI FCL study now adopted by CIGRE WGa3.16
7
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
69 kV SSCL EPRI / DOE
• SSFCL looks like a Transformer
– Tank Size - 12’h x 12’w x 12’d
• OFAF Cooling System
– Size - 10’h x 5’w x 7’d
• Total weight – 80,000 lbs
• Local / Remote Control
Outline of 69kV, 1000A, 1Ph Unit
8
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
15 kV 1200A SSCL CEC/SCE/EPRI Project
Voltage Class 15 kV
Number of phases 3
Frequency 60 HZ
Current rating 1200 A
Fault current 23 kA
Let-thru current 9 kA
Let-thru current duration 30 cycles
BIL rating 110 kV
Size 12’ H 11’ W 12’D Weight 40 000 lbs
9
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL Program Team
• DOE / Washington HQ - Gil Bindewald
• DOE / Chicago - Stephen Waslo
• EPRI Project manager - Ashok Sundaram
• Villanova University - Dr. Amy Fleischer
• SSCL Developer - Silicon Power Corp.
• SSCL Commercializer - Howard Industries
• Technical Consultant - Dr. Laszlo Guygyi
• Utility Advisor’s - Pat Duggan (ConEd)
- Pat Dilillo (ConEd)
- Sanjay Bose (ConEd)
EPRI P37D Task Force on Advanced Solid-State Substations Techniques
Chair: Jim Houston – Alabama Power Company
10
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Current Limiting Effect
2007 R&D100 Award Winner SGTO Device
- Performance Driver
11
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL Concept
• Design Features:– No cryogenics– Immediate recovery– Fail safe – No current distortions– SuperGTO
• Lower losses• Reduced Overall size and
weight• Modular design expandable to
desired Voltage & Current Ratings
Main SGTOswitchiLINE
Varistor
Line reactance
Auxiliary SGTO switch
Commutation Capacitor
Commutation Inductor
Limiting Inductor
Circuit Breaker
Operation:
• Normally the continuous current flows thru the fast speed switch (Main SGTO).
• Once the fault is sensed by high-speed sensor and declared by FPGA board, the current is commutated to Limiting Inductor (CLR).
• Introduction of CLR will limit the current to the level below the rating of the downstream breaker. The downstream breaker will trip and open the ckt within 30 cycles.
12
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
VLC – Voltage Level Controller
SSCL Architecture
13
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL Design
Standard Building Block• 44”L x 13”w x 15”h, 100 lbs
SGTO Module – 800A 5kV
Power Stack• 90”h x 66”w x 46”d• 1800 lbs
15kV 1200A Final Assembly• 11’h x 12’w x 12’d, 40,000 lbs
including Oil
14
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL Accessories
15
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL RatingsParameters 69kV 15kV
• Rated Maximum Voltage, kV rms 72.5 15.5• Rated Continuous Current, Ampere rms 1000 1200 4000• Rated Power Frequency 60 60• Available fault current, kA rms 80 23 11• Rated Let-thru Current, kA rms 40 9 5.5 • Rated Let-thru Current Duration, cycles 30 30• Rated Dielectric
– Power Frequency 1 min dry kV, rms 160 50 – Impulse, Full-wave Withstand, kV peak 350 110– Impulse, Chopped-wave Withstand, kV peak 452 142
• Ambient Temp, Degree C 40 / 50• Rated Control Power, V DC or AC, 60Hz, 1ph 125 DC 120 AC 125 DC• SSCL Power Efficiency 99.75%• Line Voltage drop 0.3%• Line Harmonic Distortion None• Partial discharge TBD 100 pC/19.5kV• Audible sound test TBD 55dBA/20’ 58dBA/6’
16
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SSCL Field Test Circuits
17
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Inherently Fault Current Limiting Cable + Stand Alone Fault Current Limiter Demonstration
Substation
Substation (new)
Generating StationStreet
Highway
Refrigeration
Fault Current Limiter
18
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
T1
CBT1SW
CBT1SE
CBT1W
CBT1ETo74440
T2
CBT2SW
CBT2SE
CBT2W
CBT2ETo74441
T3
CBT3SW
CBT3SE
CBT3W
CBT3ETo74442
T4
CBT4SW
CBT4W
CBT4ETo74443
CBT4SE
SSFCL
East 75th Street Substation
T1
CBT1SW
CBT1SE
CBT1W
CBT1ETo74416
T2
CBT2SW
CBT2SE
CBT2W
CBT2ETo74417
T3
CBT3SW
CBT3SE
CBT3W
CBT3ETo74485
York Substation
SSFCL
HTSCable
F8
SSCL Application In ConEd
One fault location
Most severe case
SSFCL in two locations
ConEd 138 kV system
equivalent from PSS/E data base
HTS cable PI circuit equivalent from
Southwire data sheet
19
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
SCE’s “Avanti” circuit a.k.a circuit of the future
VFI/Remote Controlled
Switch
Circuit Tie
Switch
Circuit Tie
Switch
Sweetwater 12KV
Northpark
12KVM
Typ. Load Transformer
ShandinSubstation
Tie RCS
RCI2
Tie RCS
Fiber Optic Duct temp Monitoring
SystemSolid State
Fault Current Limiter
Multi-Stage Capacitor Banks
TieRCS
RAR
DistributedGeneration
G
USAT
RCI3RCI
1
SCADA System Gateway
Comm.
Fiber
SEL 2100Logic Processor
Secondary Network
20
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
15kV 1200A SSCL Test Protocol
21
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
• Dielectric Test– Power frequency Voltage Withstand Test
– Full-wave lightning impulse withstand voltage tests
– Chopped wave lightning impulse withstand voltage tests
– Insulation test by power factor measurement (Dobble test)
– Insulation test by resistance measurement (Megger test)
– Partial Discharge Test
– CLR resistance & impedance measurement
• Current Limiting Test • Efficiency (power loss) Test (Steady state Operation test)• Continuous Current Carrying Test/ Temperature Test (Steady state
Operations test)• Audible sound test
Controlled Testing at KEMA Power Lab
22
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
• Tests at SSID facility:– Insulation test by power factor measurement (Dobble test)– Insulation test by resistance measurement (Megger test)– Partial Discharge test
• Tests at Shandin Sub-station:– Pre-connection testing
• Visual Inspection• Tank Pressure test• Insulation/Dielectric tests
– Insulation test by power factor measurement (Dobble test)– Insulation test by resistance measurement (Megger test)
– Field evaluation testing• Steady-State and Transient (at fault) performances
Tests at Southern California Edison
23
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Power frequency Voltage withstand Test
• Tests SSCL dielectric integrity against the continuous operatingvoltages.
• 60Hz sine-wave voltage of rated amplitude is applied for 60seconds from SSCL line terminals to ground. Leakage current is monitored
• Wet test procedure - The wet tests are made only on outdoor SSCL or on external components such as bushings, in accordance with the procedure described in IEEE Std C57.19.00-1991.
Note: For those bushings, where their voltage distribution is negligibly influenced by their surroundings, and which have been tested separately as individual bushings in accordance with IEEE Std C57.19.00-1991, the tests need not be repeated on the assembled SSCL.
24
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Power Frequency Voltage Withstand Test schematic
25
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Full-wave Impulse withstand Voltage Test
• Tests to verify their ability to withstand their rated full-wave lightning impulse withstand voltages.
• Both positive and negative, lightning impulse voltages having a peak value equal or greater than the rated full-wave lightning impulse withstand voltage shall be applied between the terminals of the SSCL and the ground / case.
• Waveform for lightning impulse tests per IEEE Std 4
Positive Impulse Negative Impulse
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© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Full Wave Impulse Test Schematic
AC
Source
27
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Chopped-wave impulse withstand voltage Test
• To verify their ability to withstand their assigned rated chopped wave lightning impulse withstand voltage.
• The voltage shall be applied to the terminals of the SSCL, without causing damage or producing a flashover, following the same procedure as for full-wave impulse test.
• The waveform and application of the chopped wave test voltage, and the type of rod gap and its location, shall be as described in IEEE Std 4-1978
28
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Schematic for Chopped Wave Impulse Test
29
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Fault Current Limiting tests
• Objective: The current-limiting test of the SSCL is to demonstrate the current-limiting performance and the related capabilities.• Test set up:
• Adjust the source impedance and voltage such that it provides Available fault current at power factor of not to exceed 5.9% lagging, equivalent to X/R = 17 at 60 Hz (11kA @ 600V for AMSC 15kV SSCL)
• Operating condition:• Run SSCL at continuous current operation and limit current at fault• Close SSCL on fault and limit the let-thru current
• Test Sequence• Pilot shot at 25% of rated let-thru fault current• Intermediate shot at 40-50% 25% of rated let-thru fault current• Final shots at 100% of rated let-thru fault current
30
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Efficiency tests
• Objective: The of the test is to evaluate the SSCL performance for power losses at various current levels.•Test conditions
• Input – At the lower end of operating voltage range and higher end of input frequency.• Output / load – At 25%/50%/75% and rated load current, and 0.85 lagging power factor.
31
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Continuous Current / Temp Rise tests
• Test conditions
• Ambient – Room temp.
• Output – 3ph bolted short.
• Input Voltage – Variable low voltage enough to provide 25% and gradual rise to 50%-75% and finally to rated load current.
• Temp. Monitoring
• Built in Heatsink temp. sensors
• Cooling liquid temp (Top, Mid, and lower level)
• Tank (top, bottom, middle on both sides)
32
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Pre-installation test
Visual Inspection
SSCL once received at site an external inspection of the SSCL tank and fittings will be done which will include the following points:
1. Is there any indication of external damage?
2. Is the paint finish damaged?
3. Are the attached fittings loose or damaged?
4. Is there evidence of fluid leakage on or around the tank coolers?
5. Are any of the bushings broken or damaged?
6. Is there any visible damage to the parts or packaging which shipped separately from the SSCL?
33
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Pre-installation test
• Tank Pressure• The tank pressure may be positive or negative when received, depending on liquid temperature. In some cases, the vacuum pressure gauge may read zero, which could indicate a tank leak. In such cases, it is recommended to contact manufacturer before installation.
• Dielectric tests• Dielectric tests are the group of tests during which the SSCL will be subjected to higher voltage levels and therefore higher voltage stresses than would normally be experienced in service. The purpose is to confirm that the design, manufacture and processing of the SSCL and insulation structure and materials are adequate to provide many years of satisfactory life.• Recommended test is power frequency voltage withstand at reduced level to 75% of rating.
34
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Field Performance Evaluation
• Objective: The objective of this test is evaluate the SSCL
performance in the field under Steady-State and transient condition
of the system in which the SSCL is connected.
•Test Monitoring:
• Steady state voltage and current sensors.
• High speed voltage and current sensors.
• Power Monitor and data recorder
• Temp. and Pressure Sensors
Steady-state and Transient Performance
35
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Field Performance Evaluation
SSCL
BYPASS SWITCH
Line
Breaker
No-load DISC.
SWITCH
SCE
15kV
LINE
SCE
15kV
LINE
Sequence of Operation: • Turn-ON: Close Bypass Switch. Close Load Disc Switch. Close Line Breaker. Open Bypass switch. Turn-on SSCL.• Turn-OFF: Turn-off SSCL. Close Bypass switch. Open Line Breaker. Open Load Disc Switch.
36
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Field Performance Evaluation
37
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Real time monitoring and analysis
• Temp. Alarm
• Pressure alarm
• Power monitoring - V, I, kVA, KVAR
• Gas relay alarm
• Fault data records
SITE REQUIREMENT:
• AC Aux Power
• Internet Access
• Working Space
38
© 2007 Electric Power Research Institute, Inc. All rights reserved.Silicon Power Corporation Proprietary
Thank you
1
Status of High Temperature Superconductor Cable and Fault Current Limiter Projects at
American Superconductor
J. F. Maguire and J. Yuan
EPRI Superconductivity ConferenceOak Ridge, TN
November 12-13, 2008
2
AgendaAgenda
• HTS Projects at AMSC• HTS Project Objectives and Milestones• Development Results of HTS Projects• Conclusions
3
HTS Projects at AMSCHTS Projects at AMSC
• Cable Projects- Transmission Voltage
• LIPA 1 (BSCCO Wires)• LIPA 2 (YBCO Wires)
- Distribution Voltage• Project Hydra Consolidated Edison
• Fault Current Limiter Project- Transmission Voltage
• Southern California Edison
4
Projects ObjectivesProjects Objectives
Demonstrate standalone HTS fault current limiter based on 2G wires in an operational power transmission grid. Introduce HV into FCL
FCL
Demonstrate HTS fault current limiting link between substations. Demonstrate feasibility of an underground installation of a fault current limiting HTS system in population condensed urban area
Hydra Project
Demonstrate a 2G HTS transmission cable and a cable joint in an operational power transmission grid. Demonstrate an FCL cable technology and repairable cryostat. Demonstrate modular refrigeration system.
LIPA 2
Demonstrate a transmission voltage level HTS cable and outdoor terminations in an operational power transmission grid
LIPA 1
5
Projects SpecificationsProjects Specifications
• 138kV/ 1200A
• Fault Current 63kA @ 4 line cycle (67ms)
• Fault Current reduction rate 36% (limit to 40kA)
FCL
• 320m long using YBCO wires
• 13.8kV/4000A, ~ 96 MVA
• Fault Current 40kA @ 4 line cycle (67ms)
Hydra Project
• 600m long using YBCO wires
•138kV/2400A, ~ 576 MVA
• Fault Current 51kA @ 12 line cycle (200ms)
LIPA 2
• 600m long using BSCCO wires
• 138kV/2400A, ~ 576 MVA
• Fault Current 51kA @ 12 line cycle (200ms)
LIPA 1
6
Projects TimelinesProjects Timelines
FCL
HYDRA
LIPA 2
LIPA 1
2012201120102009200820072006200520042003Year
7
Project PartnersProject Partners
OAK RIDGE NATIONAL LABORATORYU. S. DEPARTMENT OF ENERGY
8
LIPA 1LIPA 1
Transmission Voltage Cable ProjectLong Island Power Authority
New York
Development Results of HTS ProjectsDevelopment Results of HTS Projects
9
LIPA 1 Project TeamLIPA 1 Project Team
10
Installation SiteInstallation Site
N
Holbrook Substation
Port Jefferson Shoreham
Wading River
MillerPlace
Terryville
Centereach Superconductor
11
Major Challenges of LIPA 1 ProjectMajor Challenges of LIPA 1 Project
• System Design- 138 kV, 2,400 amp operation- Survive 51 kA @ 200 ms fault- Manage Through-Faults- Manage larger cold contraction
• HTS Conductor Design- Handle real-world cabling stress using standard manufacturing
equipment
• Termination Design- Qualify to 138 kV operation, 650 kV BIL- Safely manage voltage breakdown- Manage results from loss of cryostat vacuum
World’s First Installation of a Transmission Voltage HTS Cable
12
LIPA 1 HTS Cable SystemLIPA 1 HTS Cable System
HV Termination
RedundantCooling & Control
Cold Termination
Bul
k LN
2S
tora
ge
Heat
Pow
er
SC
AD
A
Supply
Return
13
LIPA 1 HTS Cable DesignLIPA 1 HTS Cable Design
Copper Shield Stabilization
HTS-Shield
High Voltage Dielectric
FormerHTS Tape
Inner Cryostat Wall
Outer Cryostat Wall
Outer Cable Sheath
LN2 Coolant
14
Prototype TestingPrototype Testing
• A test program has been defined together with the DOE review team based on existing standards
• Tests included- High voltage dielectric
tests - High current tests- Hydraulic tests- Load cycles- Loss measurements
Type test performed prior starting manufacturing
15
PrePre--ConstructionConstruction
16
Installation Installation -- TerminationsTerminations
• Terminations were installed with the cable phase in place
• No issues identified during termination work
17
Installation Installation -- TerminationsTerminations
• Terminations were installed with the cable phase in place
• No issues identified during termination work
18
Installation Installation -- Cable PullingCable Pulling• Cable pulling operation was tested using a 70
meter long test setup to verify method and estimate force
• Cable puling on site was achieved without issues
• Vacuum level of cryostat was checked before and after pull
• Pulling force was recorded and compared to estimated values
Cable Pulling Force
0
2000
4000
6000
8000
10000
12000
14000
16000
18000
20000
0 100 200 300 400 500 600 700
Distance [m]
Forc
e [N
]
Phase 1Phase 2Phase 3
0
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
0 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80
HTS cable distance in the PE pipe (m)
Forc
e (N
)
.
theoritical curve total (coeff0,24)therotical (rolls)
theoritical (cable in PE pipe)
19
Refrigeration substationRefrigeration substation
20
Cable cool downCable cool down
LIPA Cooldown Termination Temperature
50
75
100
125
150
175
200
225
250
275
300
0 48 96 144 192 240
Time (hours)
Tem
pera
ture
(K)
PT 101 PT 601 model model
Predicted
Actual
21
Cable Cable EnergizationEnergization• AC-High Voltage test
completed successfully- 1.5 Uo applied at each phase
for one hour- PD measurement completed
No partial discharge detected
• 24 hour dielectric soak test completed successfully
- Cable connected to LIPA grid at one end
• Cable connection at both ends completed on April 22nd
- Operation with parallel over-head line for 24 hours
- Operation without parallel path afterwards
Cable Commissioning Successfully Completed
22
Cable Operation Cable Operation -- MeasurementsMeasurements• The cable system is monitored
regarding a variety of parameters to- Ensure safe operation- Gain measurement data to
compare with design results• Measurement data analyzed so far:
- Cable cool down behavior - Cable cryostat thermal loss- Nitrogen pressure drop- Temperature increase due to
dielectric loss- Temperature increase due to AC-
loss- Thermal behavior of termination
(bushing)- Cable system time constants
Cable System Measurements in very good Agreement with Design Results
23
Steady State Operation (I)Steady State Operation (I)
0
10
20
30
40
50
60
70
80
90
7/2/08 12:00 AM 7/2/08 12:00 PM 7/3/08 12:00 AM
Tota
l MVA
0
50
100
150
200
250
300
350
400
7/2/08 12:00 AM 7/2/08 12:00 PM 7/3/08 12:00 AMPh
ase
Cur
rent
(A)
Phase RPhase SPhase T
24
Steady State Operation (II)Steady State Operation (II)
12.0
12.5
13.0
13.5
14.0
14.5
15.0
7/2/08 12:00 AM 7/2/08 12:00 PM 7/3/08 12:00 AM
LN2
Pres
sure
(bar
a)100
200
300
400
500
600
700
LN2
Mas
s Fl
ow R
ate
(g/s
)
Inlet Pressure
Return Pressure
Flow Rate
66
67
68
69
70
71
72
73
7/2/08 12:00 AM 7/2/08 12:00 PM 7/3/08 12:00 AM
Tem
pera
ture
(K)
Inlet Temperature
Return Temperature
25
Sound IssuesSound Issues
• Several questions regarding noise at the site (during operation)
• Conducted sound study- 35 db at ambient
- Source: refrigerator building
- 50 db with refrigerator running
• Acoustical Louvers- Lowered sound signature
during operation to 38 db (modeled)
26
Sound & Site MitigationSound & Site Mitigation
27
LIPA 2LIPA 2
Transmission Voltage Cable ProjectLong Island Power Authority
New York
Development Results of HTS ProjectsDevelopment Results of HTS Projects
28
LIPA 2 Project TeamLIPA 2 Project Team
29
Major Challenges of LIPA II ProjectMajor Challenges of LIPA II Project
• System Design- Integrate single phase fault current limiting phase into the existing
system
• 2G HTS Conductor Design- Address real-world cabling stress using standard manufacturing
equipment
• Cable Design- Demonstrate field joint- Demonstrate field reparable cryostat
• Develop a 20 KW modular high efficiency refrigerator
30
LIPA II HTS Cable SystemLIPA II HTS Cable System
Existing HV Termination
RedundantCooling & Control
Existing Cold Termination
Bul
k LN
2S
tora
ge
Heat
Pow
er
SC
AD
A
Supply
Return
Replacement 2G Phase
Field Joint
31
LIPA 2 HTS Cable ConceptLIPA 2 HTS Cable Concept
Copper Shield Stabilization to be removed
HTS-Shield
High Voltage Dielectric
Cable conductor has to be redesigned for thermal contraction (and current limiting)
Inner Cryostat Wall
Outer Cryostat Wall
LN2 Coolant
32
LIPA 2 WireLIPA 2 Wire
• YBCO Coated Tapes- Lower Tc, higher resistance substrate: Can be made to
be current-limiting- Different dimensions and physical properties:
• YBCO coated onto one side of buffered Ni-W substrate
• Brass laminated onto both sides• ~ 0.3 mm thick, splices even thicker
• Splices are being developed
33
Cable design and manufacturing processCable design and manufacturing process
• Dummy cable approach to develop the cable design
- Develop cable design based on modified modeling tools
- Manufacturing of short samples • Measurement of electrical
characteristics (AC-loss)- Manufacturing trials using industrial
machine adapted to HTS tape stranding- Testing of samples in terms of mechanical
and high voltage aspects
• Status- Two different design options considered- First manufacturing trials (dummy cables)
focus on one of the two designs
34
Dummy cable 01 Dummy cable 01 -- Current StatusCurrent Status
• Hollow flexible former- Dummy cable is being produced now- Superior concept
• Only small force due to thermal contraction• Small cross-section, stainless steel:
• High resistance, good for current limitation - Requires some effort due to flexibility of former in the
machine- Preferred design
35
High Voltage TerminationHigh Voltage Termination
• LIPA 1 terminations design is kept for this project but adapted for the new YBCO HTS cable:
- Removal of the cable termination shrinkage management (blocking of the cable)
- Adaptation of the cable connection for 2G wires
• Status:- Updating of the cable connection is in progress with different new brazing alloys
studied- Continuation of the development required now some LIPA 2 cable samples in order
to achieved some connection and mechanical tests and improved the components
36
High Voltage TerminationHigh Voltage Termination
• LIPA 1 terminations design is kept for this project but adapted for the new YBCO HTS cable:
- Removal of the cable termination shrinkage management (blocking of the cable)
- Adaptation of the cable connection for 2G wires
• Status:- Updating of the cable connection is in progress with different new brazing alloys
studied- Continuation of the development required now some LIPA 2 cable samples in order
to achieved some connection and mechanical tests and improved the components
37
Superconducting Cable JointSuperconducting Cable Joint
• HTS cable joint- Develop and test a straight joint to connect
superconducting cables• Design of conductor connection• Design of joint dielectric insulation• Design of screen connection• Design of joint cryostat
• Cryostat for subscale test• Cryostat for on site installation
- Full prototype test of cable joint in the laboratory- Installation of a single cable joint on site
38
Status: High Voltage JointStatus: High Voltage Joint
• A first joint design has been set up considering two main physical constraints- Thermal: no overheating in the central cable connection with nominal current (not in
direct contact with liquid nitrogen)
- Electrical: E field management in an optimum dimension of the joint
• Prototypes for testing assembly procedures successfully prepared and tested with nominal current in LN2 (temperature measurement)
39
Status: High Voltage JointStatus: High Voltage Joint
• The first design of the joint has been assembled in NEXANS Hanover testing laboratory in June/July 2008
• First results on this component achieved in September 2008• AC withstand test 190 kV / 30 min• Lightning impulse test 650 kV (+/-)• Partial discharge measurement
40
Inlet Termination(Connection to the Transformer)
Outlet Termination with the Joint inside
25 m Coated Conductor Cable
Joint in the Test FieldJoint in the Test Field
41
Field Repairable CryostatField Repairable Cryostat
• Field repairable cryostat- Perform optimization study to determine
cryostat vacuum barrier distance based on - Develop and demonstrate vacuum barrier
manufacturing techniques- Develop improved thermal insulation system to
perform under repair vacuum conditions- Demonstrate field repair in laboratory
• Status of work- Vacuum barrier manufacturing techniques
• Various designs developed- Improved thermal insulation system
• Investigation of vacuuming behavior of alternative thermal insulation materials
42
Modular Refrigeration System ObjectiveModular Refrigeration System Objective
Develop a new Refrigeration technology dedicated to long-length HTS cable with the main characteristics below
- Low operation cost• High efficiency
• Low maintenance
- Low refrigerator cost• Simple design
• Modular design
- High reliability
- Long lifetime
43
Refrigeration System ObjectiveRefrigeration System Objective
Develop a new Refrigeration technology dedicated to long-length HTS cable with the main characteristics below
• Liquid nitrogen delivered 72 K
• LN2 pressure drop 3 bars
• Cold power 120 kW total - 20 kW Modules
• Efficiency > 20% Carnot
• Cooling Air cooling (-20 / 50°C)
• Manufacturing cost target <$100/cold W series production
44
Refrigerator Development Status (Phase 1)Refrigerator Development Status (Phase 1)
Progress made thus far- Thermodynamic analyses of reverse Turbo-Brayton cycle Completed
- Cooler configuration scenarios Identified
- Numeric modeling of cooler configuration and
Refrigeration sub components Completed
- Model validation Completed
- Creation of a numerical model for each cooler configuration Completed
- Optimization of each cooler configuration Underway
45
Project HydraProject Hydra
Distribution Voltage Cable ProjectConsolidated Edison
New York City
Development Results of HTS ProjectsDevelopment Results of HTS Projects
46
Team Roles and ResponsibilitiesTeam Roles and Responsibilities
SouthwireAMSC
Cable and Accessory Design
Cable Manufacturing
Cable and Accessory Installation
Utility Requirements
Project Oversight
HTS FCL Cable System Site
System Hardware Development
Wire Development
Wire Manufacturing
Project Management
Technical Oversight
System Design
AMSCPrime Contractor
DHSS&T Division
ORNL
Con Edison
Technical Support
50m Prototype Cable Test Site
Air Liquide
Altran Solutions
47
Installation SiteInstallation Site
World’s First FCL Distribution Cable to be Installed in Operating Grid
48
Program StructureProgram Structure
Phase 1System
Development
Phase 1AFault Current Limiting
Cable technology
Phase 1BStand-Alone Fault Current
Limiting Technology
Phase 2System Installation
ORNL50 Meter Test and Technical Support
DHS/ HYDRACurrently ExecutingPlanning
49
HYDRA HTS Cable SystemHYDRA HTS Cable System
Supply
Return Refrigerator
PowerHeat
HTS Cable
Return Line
50
138kV Transmission Bus
13.8kV Distribution Bus
Substation #1138kV Transmission Bus
13.8kV Distribution Bus
Substation #2
HTS Fault-Current Limiting CableFast Switch
(Circuit Breaker)
Reactor Conventional Copper Cable
To Loads To Loads
Secure Super GridsSecure Super Grids™™ TechnologyTechnology
Note: Red breakers are ClosedGreen breaker is Open
51
Cable DesignCable Design-- TriaxTriaxTMTM by by SouthwireSouthwire
HTS LayersHTS Layers
Hollow FormerHollow Former
DielectricDielectric
CryostatCryostat
ShieldShield
52
3 m Cable FCL Tests3 m Cable FCL Tests
• The prospective fault current of 60 kA was reduced to 44 kA on the first ½ cycle to < 30 kA at the end of the 140 ms duration fault
• A perspective 140 ms fault current of 44 kA was reduced to 29 kA
• The voltage developed due to the heating was 8-11 V/m over the 140 ms duration fault
• This was comparable to the design fault of 300-m cable which results in ~ 10 V/m
• Measured temperature increase to 85-95 K
• Re-cooling time to 77 K is 9 min
• No change in temperature measured after a 9.1kA, 270ms through fault test
• No change in temperature or voltage after a 2000 ms, 7.2kA overload test (1.8X)
53
3m Cable FCL Tests3m Cable FCL Tests
54
3 m Cable FCL Tests3 m Cable FCL Tests
55
Refrigerator RequirementsRefrigerator Requirements
• Refrigeration Cycle chosen is the Reverse-Brayton- Best suited technology for high power applications (> 6 kW)- Best return on specific efficiency (We/Wc) vs. capital cost
• Flexibility Requirement:- 80% of time at 50% heat load on HTS cable
• Reliability - Redundancy accomplished at component level: compressors,
pumps, expanders, electronics, instrumentation- No 1st order single point of failure allowed
• Capacity Margin- Current design has 50% safety margin to the expected losses
56
Reverse BraytonReverse Brayton--Cycle HardwareCycle Hardware
- Estimated foot print size & weight• 13 m x 7 m ( 42’ x 25’ ) + roof for cooling water exchanger• ~ 24 000 kg ( 53 000 lbs ) empty• Fits within available space
57
FCL ProjectFCL Project
Transmission Voltage FCL ProjectSouthern California Edison
California
Development Results of HTS ProjectsDevelopment Results of HTS Projects
58
Team Roles and ResponsibilitiesTeam Roles and Responsibilities
SiemensAMSC
FCL Module and Accessory Design
FCL Manufacturing
FCL Module and Accessory Installation
Utility Requirements
Project Oversight
HTS FCLSystem Site
System Hardware Development
Wire Development
Wire Manufacturing
Project Management
Technical Oversight
System Design
AMSCPrime Contractor
DOE
SPE - SCE
SCE
Air Liquide
Nexans
HV Termination
HV Consulting
59
SuperLimiterSuperLimiterTMTM Demonstration SiteDemonstration Site
The Valley Substation is selected
• Selection criteria- Voltage- Transmission planning- Civil engineering
• Valley Substation selected
• Located near Riverside, CA in a desert climate
• Analysis used to select bus tie application
• Significant load growth planned over the next 10 years
- Tapped external reactor enables device to easily adapt
RiversideRiverside
Valley Valley SubstationSubstation
60
SCE ProfileSCE Profile
•• 50,000 Mile50,000 Mile22 Service TerritoryService Territory
•• 120 years of service120 years of service
•• $17 Billion T&D Assets$17 Billion T&D Assets Distribution•• 85,000 Circuit Miles85,000 Circuit Miles•• 690,000 Transformers690,000 Transformers
Customers•• 4.7 Million Meters4.7 Million Meters•• 13 Million 13 Million
CustomersCustomers•• 22,889 MW Load22,889 MW Load
Transmission•• 12,600 Circuit Miles12,600 Circuit Miles•• 4,200 Transformers4,200 Transformers
SCE is one of the largest utilities in the United States
61
SuperLimiterSuperLimiterTMTM Southern California EdisonSouthern California Edison• SCE is investing in the future
- > $3 billion invested in T&D over the last five years- $11 billion planned infrastructure investments over the
next decade.• SCE has considerable experience with
superconducting Fault Current Limiters- Since 1993 in DOE-SPI, tested a 15kV FCL in 1999- SCE role in this program is
• Specifying requirements • Providing the prototype operation site
• 138 kV Transmission Voltage level FCL addresses - Elimination of CB and other equip. replacement- Enhanced reliability, shorter customer outages- More stable, higher-quality electricity supply- A “self-healing” grid July 1999: FCL at a Southern California
Edison substation
SCE has unique experience with HTS FCL technology and this program extends this to transmission voltage levels
62
SuperLimiterSuperLimiterTMTM Major ElementsMajor Elements
InsulationInsulationStainless StripStainless StripHTS FilmHTS FilmNiW StripNiW StripSolderSolder
1.2 cm insulated HTS tape 1.2 cm insulated HTS tape based on standard insertbased on standard insert
Cryostat sized for Cryostat sized for modular expansionmodular expansion
Design based on validated components is designed for modular expansion
Cooling System Similar Cooling System Similar to Navy Motor Programto Navy Motor ProgramN+1 RedundancyN+1 Redundancy Bifilar 2.2 MVA medium voltage Bifilar 2.2 MVA medium voltage
module tested Jan. 2007module tested Jan. 2007
Valley Valley SubstationSubstation
138kV termination in 138kV termination in operation at LIPA siteoperation at LIPA site
63
FCL Operating PrincipleFCL Operating Principle
FCL system operation is based on simple operating principles
Reactor
Normal State Resistance
Virtual SwitchSuperconductor
Physical Switch
Supply Bus
Load Bus
Under normal conditions, power flows through superconductor with virtually no impedance and system is electrically “invisible”
During fault conditions, superconductor becomes resistive and with reactor, limits current
Physical switch opens
to protect FCL system;
reactor maintains
current
Shortly after fault clears, power resumes flow through superconductor
64
Basic SpecificationsBasic Specifications
As required by customer
1.6puTrip Current
As required by customer
40kASite Limited Current
>80kA63kAMaximum Site Unlimited Fault Current
>2,000A1,200ANominal Current
138kV138kVInsulation Class
115-138kV115kV rmsNominal Voltage
Production Units
Prototype System
Requirement
Team has approved a working specification for system
Refrigeration System
Power Heat
FCL Vessel Assembly
Protection and DAQ System
ReactorSized to Limiting Requirements
Opening Switch
Source
Load
SwitchControl
65
SuperLimiterSuperLimiterTMTM Operating ConditionsOperating Conditions
•Constraints-No bubbles around the bottom of bushing – sub-cooled LN2-Termination dielectric requirement P > 3bar-Fast recovery time – saturated LN2
•Solution-Operate FCL in sub-cooled LN2 with nominal operating temperature lower than design point.• FCL design at temperature 74K@5bar(a), but operate at temperature 72K@5bara
• Temperature margin determines the number of faults the system can absorb before system is off-line to re-cool
• 2K margin allows LN2 to absorb 57MJ energy (~6 faults)• 5 bar pressure will allow LN2 in coil vicinity absorb fault energy without bubbling
FCL operates at high pressure sub-cooled LN2 temperature
Refrigeration System
Power Heat
FCL Vessel Assembly
66
SuperLimiterSuperLimiterTMTM Refrigeration SystemRefrigeration System
Pressure
Level
Level
6000Planned Capacity4250Total Max. Predicted1950AC Losses
350Lines, Valves, Bayonets
900Terminations
200Other Refrig. System
850Cryostat
Value (W)Heat Load
• AMSC has operated HTS systems in utility/harsh industrial conditions- LIPA and TVA/SuperVAR Project
• DOE-FCL system based on lessons learned in those systems- Phase 1b – open cycle option shown above- Phase 2 - replace with closed cycle modification
• Simplified, COTS based system• Significant margin planned for prototype system
Refrigeration based on experience at LIPA and other AMSC utility HTS systems
67
SuperLimiterSuperLimiterTMTM Test SiteTest Site
Bus TieBus Tie115 KV 115 KV Outgoing Outgoing FeederFeeder
1000 MW 1000 MW Future GenFuture Gen
Inland EmpireInland Empire
115 kV115 kV
115 kV115 kV
500 kV500 kV
115 kV115 kV
“A”“A” “B”“B”
“C”“C” “AB”“AB”
SerranoSerrano500 kV500 kV
Devers Devers 500 kV500 kV
(Studied)(Studied)(Selected)(Selected)
A bus tie application at the Valley Substation is selected
Present Installation:• 4-3Phase, 336/448/560 MVA
525-120 kV, OA/FOA/FOA Transformers.
• Sectionalized 115 kV bus -each section fed by 2 transformers
• Max. single-phase-to-ground fault = 30 kA
• All 115 kV CBs rated 40 kAPlanned Future Installation:• Load growth in the area and
interconnection of new generators will require additional transformers
• Fault current duty will rise above 40 kA
68
SwitchingSwitching Module Module forfor thethe HV SFCL ProjectHV SFCL Project
Main design characteristics• The switching module comprises
3 parallel x 17 series = 51 bifilar pancake coils per phase
• Two in hand winding with 12 mm wide wire to increase the current
• Improved electrical strength due to:- Insulated wire- New contact design- Corona rings around the coils
• Horizontal stack with radial supports between module and cryostat wall
Regions stressed by BIL tests, numbering see next slide
Alternating current directions between adjacent turns of bifilar coils cancel most magnetic fields
(1)(1)
(1)(1) (2)(2)
(3)(3)
69
Performance Modeling and TestingPerformance Modeling and Testing
Switching• First tests on a 3 m sample of 12 mm wide HTS-wire:
Critical current 167 A @ 77 K, 258 A @ 72 K
• More than 60 switching test in saturated (77 K) and sub-cooled (72 K, 1.2 bar) LN2
0 10 20 30 40 50-2000
-1000
0
1000
2000
-400
-200
0
200
400
Time (ms)
Cur
rent
(A)
Volta
ge (V
)
T: ~72 K
77 K, 77 K, satsat., t: 100 ms., t: 100 ms
72 K, 1.2 bar, t: 500 ms72 K, 1.2 bar, t: 500 ms
70
Performance Modeling and TestingPerformance Modeling and Testing
Recovery time• About 12 - 15 sec measured on full size dummy coil in sub-cooled LN2
• 12 mm wide dummy wire insulated with wrapped Teflon tape• Amount of LN2 available for cooling restricted by appropriate enclosure
to simulate adjacent coils
-0.05 10 2060
70
80
90
100
110
0
T: 77 K, p: 1 bar T: 72 K, p: 1.2 bar
Res
ista
nce
ratio
(%)
Time (s)
71
FCL FCL TerminationTermination Design ValidationDesign Validation• AC withstand test successfully completed according IEC 60840
- 190kV / 30 minutes
• Partial Discharge measurement sucessfully completed (IEC 60840)- Voltage increase up to 140 kV for few minutes- Decreasing to 114 kV and measurement- No PD measured (noise level < 3pC)
• Lightning impulse test successfully completed (IEC 60840)- 650 kVp (10 shots in both polarity)
• Switching impulse successfully completed based on IEEE C57.12.00:- Success of the test (540 kVp 250/2500µs – both polarity)
FCL termination high voltage design successfully validated
72
SummarySummary
• AMSC is currently advancing the state of the art in HTS power products
- Worlds First Transmission Voltage HTS Cable in Operation
- Worlds First Fault Current Limiting Cable for use in a distribution grid under development
- Transmission Voltage Fault Current Limiter under development
superior performance.powerful technology.
SuperPower, Inc. is a subsidiary of Royal Philips Electronics N.V.
Transmission Level HTS Fault Current Limiter
Chuck Weber
8th Annual EPRI Superconductivity ConferenceOak Ridge, TN November 12, 2008
8th Annual EPRI Superconductivity Conference – November 12, 2008
SFCL program overview
15.248"
7.362"
15.248"
7.362"
138 kV, 650 kV BIL Bushings
Vacuum Vessel
Pressure Vessel
Matrix Assembly
Inner diameter
Inner Height
HTS Assembly Height
Assembly diameter
Partners
Specifications• YBCO based, resistive type FCL• 138 kV class device• Fault Current – 13.8 kA• Load Current – 1,200 Arms• Design fault current – 37 kA• Design device response – Recover
to superconducting state after a fault carrying full load current
8th Annual EPRI Superconductivity Conference – November 12, 2008
Generalized SFCL Specification Development
• Baseline Design for Program was the AEP SPORN substation site– This is a niche application site, operating at 400Arms, 138 kV– Prospective fault current 26 kArms (~90 kA peak) and 13.8 kArms
(~ 37 kA peak)
• Working with AEP, we have identified a site with broader generalapplication
– TIDD substation– 1,200 Arms, 138 kV– Prospective fault current is 13.8 kArms (~37 kApeak)
8th Annual EPRI Superconductivity Conference – November 12, 2008
TIDD Substation – (Partial) One-Line Diagram
Proposed SFCL Installation Location
8th Annual EPRI Superconductivity Conference – November 12, 2008
Prior accomplishments
• Proof-of-Concept demonstrated– MCP 2212 (2004)– 2G YBCO (2006)
• Beta device testing specifications established
• Completed design and testing of HV bushings (SEI)
• Investigated several ‘engineered’ 2G architectures for improved RUL
• Design and laboratory testing of shunt coils to withstand high fault transient loads
• Thermal simulation of RUL process• Weibull plots of ‘standard’ 2G failures• Conceptual CRS & vessel design• Investigated LN2 dielectric properties
2G FCL - Probability of failure for 2G tapes as function of energy input
0.01
0.1
1
10
100
20 25 30 35 40 45 50
Energy [J/cm/tape]
Prob
abilit
y of
failu
re [%
]
Probability of Failure - Test dataProbability of Failure Calculated using Weibull Distributuon
8th Annual EPRI Superconductivity Conference – November 12, 2008
Improvements to shunt coil and contact design
• Shunt coil improvements:– Manufacturing improvements
(easier assembly, more robust coil)
– Mechanical strength – Multi-Layer winding (size
reduction)• Connector improvements:
– Shape optimization to avoid contact hotspots
– Improvement in RUL Time– Improvement in RUL Current– Improvement in consistency of
contact resistance
8th Annual EPRI Superconductivity Conference – November 12, 2008
Tape heating near contact during fault impacts RUL
8th Annual EPRI Superconductivity Conference – November 12, 2008
Correlation between different contact geometries
Total Current (80A peak)
Recovery Voltage
Superconductor’s Current
Straight Thick Contacts(M3-460 Tape):I load = 80 A
RUL = 82 sec.
Total Current (80A peak)
Recovery Voltage
Superconductor’s Current
Total Current (80A peak)
Recovery Voltage
Superconductor’s Current
Straight α-Tapered Contacts(M3-460 Tape):
I load = 80 A RUL = 3.5 sec.
Straight β-Tapered Contacts(M3-460 Tape):
I load = 80 A RUL = 2.8 sec.
8th Annual EPRI Superconductivity Conference – November 12, 2008
Recent KEMA tests• Recent rounds of KEMA testing focused on critical AEP reclosure sequence on
an HTS element
• Straight elements were used
• Improved connector designs were used
• “Standard”, pre-qualified tapes were used
• Test Dates: May 2008, July 2008
5 CyclesFault
13kA/7kA
18 Cycles Load Current
15 sec Load Current
135 sec Load Current
5 CyclesFault
13kA/7kA
5 CyclesFault
13kA/7kA
5 CyclesFault
13kA/7kA
Breaker opens and locks-out
Recovery under NO Load Current
5 CyclesFault
13kA/7kA
160 sec Load Current
8th Annual EPRI Superconductivity Conference – November 12, 2008
2G RUL capabilities tested at KEMA
• ‘Standard’ SF12100 2G wire used
• Test conditions- 37 kA fault
- follows AEP sequence
• Test variables- Shunt impedance
- Number of parallel tapes
- System voltage (v/cm/tape)
- Load Current
16 Tapes8 Tapes
4 Tapes100V
200V
250V
300V
0
50000
100000
150000
200000
250000
Load Pow er (VA)
Total Recovered Power, 2x5 cycles Faults at 37kA with 10 mOhm
Parallel Tapes
Voltag
e
8th Annual EPRI Superconductivity Conference – November 12, 2008
3 x Base-Line Voltage
w/o Load
w/ Load
Achieving RUL is a difficult task
Without load current recovery is very fast
Adding load current makes recovery much more difficult
8th Annual EPRI Superconductivity Conference – November 12, 2008
Base-Line Voltage
RUL
1.5 x Base-Line Voltage
RUL
3 x Base-Line Voltage
RUL
Electrical stress on the tapes can limit RUL
• RUL time can affected by increasing the V/cm on the tape
• Limits of the design optimization are understood
8th Annual EPRI Superconductivity Conference – November 12, 2008
Factors impacting RUL defined by test results
1.67 m-Ohm
5 m-Ohm
100 V200 V
250 V300 V
0
10000
20000
30000
40000
50000
60000
70000
80000
Load Power (VA))
Total Recovered Power, 2x5 cycles Faults at 37kA with 4 Tapes
Shunt ImpedanceVoltage
Sample surface plot of RUL conditions
8th Annual EPRI Superconductivity Conference – November 12, 2008
Ability to predict RUL over wide design space
1.67
m-O
hm
5 m
-Ohm
4Tap
es, 1
00V
4Tap
es, 2
50V
8Tap
es, 1
00V
8Tap
es, 2
50V
16Ta
pes,
100
V
16Ta
pes,
250
V
0100200300
400500
600
700
800
900
1000
Maximun Recovered Load Current
Recovered Current with 2 Asymmetrical 37kA Faults, 5 cycles each
ImpedanceVoltage, #Tapes
Maximum Load Current as a function of shunt impedance, operating voltage & number of tapes
8th Annual EPRI Superconductivity Conference – November 12, 2008
RUL with 90% of the Power recovered within the 2nd and the 3rd 37 kA Faults
Worst case conditions at Tidd can achieve RUL
Full recovery expected with optimal bath conditions
8th Annual EPRI Superconductivity Conference – November 12, 2008
Bath Conditions Impact on Ability to Recover
100 150 200 250 300 350 400 450 500 5500
100
200
300
400
500
600Heat OutHeat In
No Recovery Due to Film Boiling
Temperature (K)
Pow
er (W
)
Lowering the shunt coil value or increasing the resistance of the stabilizer layer will help with film boiling.
Lower Zshunt, Higher Ztape
Boiling Heat Transfer for LN2
0.1
1.0
10.0
100.0
1.0 10.0 100.0 1000.0
Twall - Tsat (K)
q/A
(W/c
m2 )
During the fault transient, tape heats up to film boiling region. Bath conditions (pressure, subcooling) shift boiling heat transfer curveBath conditions have an impact on the dielectric strength of LN2
8th Annual EPRI Superconductivity Conference – November 12, 2008
Bath Conditions Impact on Ability to Recover
Boiling Heat Transfer for LN2
0.1
1.0
10.0
100.0
1.0 10.0 100.0 1000.0
Twall - Tsat (K)
q/A
(W/c
m2 )
Once film boiling threshold is crossed, nucleate boiling ensues Bath conditions (pressure, subcooling) shift boiling heat transfer curveBath pressure shifts saturated boiling temperature, limiting nucleate boiling recovery
75 80 85 90 95 1000
100
200
300
400
500
600Heat OutHeat In
No Recovery Due to Nucleate Boiling
Temperature (K)
Pow
er (W
)
Lowering the operating pressure will help with nucleate boiling, but decreases dielectric properties
Lower pressure
8th Annual EPRI Superconductivity Conference – November 12, 2008
Modeling indicates where operating conditions for successful RUL exist
Recovery Under Load vs Number of Tapes
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
0 2 4 6 8 10 12 14 16
Number of Tapes per Element
Rec
over
y Lo
ad C
urre
nt (a
rms)
Baseline
Pressure = 0.5 atmTbulk = 71.922 K
Pressure = 0.5 atmTbulk = 71.922 KStabilizer = 1% AgAu
Pressure = 0.75 atmStabilizer = 1% AgAu
Pressure = 0.75 atmStabilizer = 2.2% AgAu
Baseline Shunt = 5 mΩ/m
Baseline Shunt = 7.5 mΩ/m
Baseline - Substrate = 4 mil Stabilizer = Ag Shunt Coil = 10 mΩ/m No dielectric coating Ic @ 77 K = 250 amps n-value = 20 Pressure = 1 atm Tbulk = 72 K
19 Managed by UT-Battellefor the Department of Energy DOE Peer Review 2008
Introducing bubbles in LN lowers breakdown strength: FCL recovery
• Two experiments– Open bath LN– Pressurized cryostat
• Nitrogen gas provided by fused silica capillary tube
• Varied flow rates• Parallel plane profiled
SS electrodes• BD strength of LN is
~5x the gas at 1 bar
Bubbles form thermally or electrically and can affect the breakdown strength
2 mm gap0.5 mm capillary tube
Important for FCL Recovery under Load
20 Managed by UT-Battellefor the Department of Energy DOE Peer Review 2008
Effect of externally provided bubbles on LN Breakdown: AC breakdown
all data w and w/o bubbles
Breakdown Field (kVrms/mm)5 6 7 8 9 20 3010
Cum
ulat
ive
Failu
re P
roba
bilit
y (%
)1.0
5.0
10.0
20.030.040.050.060.070.080.090.095.099.099.9
Effect of Bubbles
Presence of bubbleswithout bubbles with bubbles
Aver
age
Elec
tric
Fiel
d (k
Vrm
s/m
m)
0
2
4
6
8
10
12
14
16
18
Liquid nitrogen at 1 bar
• Bubbles in LN lowers breakdown strength• Change in slope at lower probability indicates change in BD mechanism
8th Annual EPRI Superconductivity Conference – November 12, 2008
Summary
• Significant progress in understanding and impacts of:– RUL
• Variables impacting RUL studied and understood• Worst case conditions at TIDD can be met• Impact of device design and cost under evaluation
– LN2 Dielectrics• Impact of bubbles on breakdown mechanism and dielectric
strength
• Loss of cryogenic partner a setback, but not fatal• Next step: Alpha detailed design
8th Annual EPRI Superconductivity Conference – November 12, 2008
Thank You for your attention!
For more information:
www.superpower-inc.comor
superior performance.powerful technology.
SuperPower, Inc. is a subsidiary of Royal Philips Electronics N.V.
Status Update for the Albany HTS Cable ProjectC.S. Weber (SuperPower)
8th Annual EPRI Superconductivity ConferenceOak Ridge, TN November 12, 2008
9th Annual EPRI Superconductivity Conference – November 12, 2008
Program Overview– 350m long - 34.5kV - 800Arms - 48MVA– Cold dielectric, 3 phases-in-1 cryostat, stranded copper core design– Two Phases – Phase I - 320m + 30m BSCCO
– Phase II - 30m BSCCO replaced by 30m YBCO cable
Supported by Federal (DOE) and NY State (NYSERDA) Funds
Design, construct and operate the Cryogenic Refrigeration System, and provide overall cable remote monitoring and utility interface
Design, build, install, and test the HTS cable, terminations, & joint
Host utility, conventional cable & system protection, system impact studies
Project Manager; Site infrastructure, Manufacture of 2G HTS wire
9th Annual EPRI Superconductivity Conference – November 12, 2008
Site Location
Phase II: 30m YBCO
Phase I: BSCCO
9th Annual EPRI Superconductivity Conference – November 12, 2008
System Protection Philosophy
• Worst case fault conditions – 23 kA rms (33 kA peak)• Multiple levels of relay & breaker protection
– Primary - RFL-9300 charge comparison relays (87L) – 8 cycle clearing time– Secondary - SEL-311B relay packages – 8 – 38 cycle clearing time
• Breaker failure protection– Will initiate fault clearing by tripping breakers on associated Menands or Riverside 34.5kV bus– cleared in 20 to 50 cycles (0.33 to 0.83 sec)
• System monitoring @– BOC Remote Operating Center– NM Eastern Regional Control Center
9th Annual EPRI Superconductivity Conference – November 12, 2008
Advantages of the 3-in-One CableDesign
• Compact size (O.D. = 135mm) (5.3”)
• Nearly perfect magnetic shielding
– > 95% cancellation of field
• Significant reduction of contraction forces due to ‘slack’ winding
• Excellent fault current protection
– Cable remains superconducting at worst case fault condition, survives extended duration (2nd
contingency) fault without damage
Albany HTS Cable Design
HTS Conductor( 2-layer)
HTS Shield( 1-layer)
Cu Shield
135 mm35 mm
Electrical Insulation( PPLP +Liquid Nitrigen)
Cu Stranded Former
Tension Member
Stainless Steel Double Corrugated
Cryostat
HTS Conductor( 2-layer)
HTS Shield( 1-layer)
Cu Shield
135 mm35 mm
Electrical Insulation( PPLP +Liquid Nitrigen)
Cu Stranded Former
Tension Member
Stainless Steel Double Corrugated
Cryostat
9th Annual EPRI Superconductivity Conference – November 12, 2008
Cryogenic Refrigeration System: Approach
Cryocooler
Thermosyphon
Liquid NitrogenStorage/buffer
Subcooled liquid nitrogen loop
HTS cable
Hybrid arrangement permits transparent use of bulk liquid nitrogen for back-up
Thermosyphon provides common heat exchange interface between cable and open or closed refrigeration sources
Advantages:- excellent reliability/cost ratio- compact footprint- flexible ‘plug & play’ design- good efficiency
9th Annual EPRI Superconductivity Conference – November 12, 2008
Minimum CRS Requirements & Cold Box Arrangement
1.4 m
1.6 m
BOC
Item Specification
Coolant supply temperature 67 to 77 KTemperature stability +-0.1 K - normal operation
+-1.0 K - backup operationRefrigeration capacity 5 kW at 77 K
3.7 kW at 70 KMinimum coolant pressure 1 to 5 barg +-0.2Maximum coolant flow rate 50 liter/min +-1
(excluding CRS)
9th Annual EPRI Superconductivity Conference – November 12, 2008
Post-Cable Testing: Cryogenic System Step Response
60
62
64
66
68
70
72
74
76
78
80
0 1 2 3 4 5 6 7 8 9 10 11 12 13
Time (hours)
Tem
pera
ture
(K)
0
5
10
15
20
25
30
Coo
ling
Pow
er (K
w)
Coolant return
North Termination
South Termination
Coolant Supply
Refrigeration power
Hybrid operation
3 Kw nominal
8 Kw peak
+ - 0.05K
+ - 0.10K
Pre-energization: 3 Kw nominal. Post-energization: 3.1-3.3 kW nominal overall heat load
9th Annual EPRI Superconductivity Conference – November 12, 2008
66
67
68
69
70
71
7/20 8/17 9/14 10/12 11/9 12/7 1/4 2/1 3/1 3/29 4/26
Date (2006-2007)
Tem
pera
ture
[K]
0
4
8
12
16
20
Tran
smitt
ed E
lect
ricity
[MVA
]
Cable Inlet Temperature
Cable Outlet Temperature
Transmitted Electricity
Chiller System ShutdownSupply Voltage Issue
Energizedon July 20,2006
Completedon May 1, 2007
Fault Current Event
7kA
8 cycle
The HTS cable system was checked for damage after the fault eventNo Issues Re-connected to Power Grid
More Than 6,700 Hrs of Reliable Power Transmission
Summary of Phase I Operation
9th Annual EPRI Superconductivity Conference – November 12, 2008
-200
-150
-100
-50
0
50
0 100 200 300 400 500 600 700 800Position [m]
Tem
pera
ture
[ ]
30m HTS Cable320m HTS Cable
350m Return Pipe
12H
1D
3D
5D
7D
9D
11D
14D
21D
SouthTerm
NorthTerm
Before warming-up,• Megger Test• Ic Measurements
Warm-up Process,(1) LN2 pumped into the CRS bulk storage tank(2) Remaining LN2 in system allowed to evaporate naturally
No Change
Vacuum level• No leakage
Cable Tension• Returned to theoriginal value
(approx. 200kgcompressive force)
Commencement of Phase II
9th Annual EPRI Superconductivity Conference – November 12, 2008
1 Meter Cable Characterization (after removal)
-50
0
50
100
150
200
0 200 400 600 800 1000 1200
I(Amperes)
V(uVolts)
Contact #2 R=32 uohms
Contact #1R = 6 uOhms
0
10000
20000
30000
40000
0 500 1000I(Amperes)
V(uV)
Contact resistance measurements were performed in the superconducting state T=75.5K
• The critical current of the inner layer with 12 strands of superconductor was measured at 75.5K in self field.
• Distance between voltage taps = ~75cm• Ic = 965Amperes @ 1μV/m• 1100A @ 1μV/cm
• Contact was made to 12 strands with single strand Ic(B=sf, 75K) ~ 92 amperes
*Data courtesy of Yates Coulter, LANL
9th Annual EPRI Superconductivity Conference – November 12, 2008
2G wire cable winding
3 core stranding
In 2007, 30 m cable was manufactured by Sumitomo Electric with ~10,000 m of SuperPower 2G HTS wire
Cu StrandedWire Former
Electric Insulation(PPLP + Liquid Nitrogen)
Stainless Steel DoubleCorrugated Cryostat
Cu Shield2G HTS wire(2 shield Layers)
2G HTS wire(3 conductor Layers)
135 mm
9th Annual EPRI Superconductivity Conference – November 12, 2008
Summary of 30 meter YBCO Cable Shipping Tests
• Manufacture of 30m YBCO cable completed in March 2007
Critical Current• Conductor : 2660 – 2820A (DC) at 77K• Shield : 2400 – 2500A (DC) at 77K
AC Loss• 0.34W/m/phase at 0.8kArms, 60Hz
Bending Test (18D: Bending Dia. = 2.4 m)• No Ic degradation• No defect was found at dismantling
Inspection
Voltage tests (Based on AEIC)AC 69kV for 10 minute,
Imp ±200kV, 10 shots/eachDC 100kV for 5 minutes
The following shipping tests were conducted successfully on samples from long cable:
9th Annual EPRI Superconductivity Conference – November 12, 2008
-0.5
0
0.5
1
1.5
2
0 500 1000 1500 2000 2500 3000Current (A, DC)
Elec
trica
l Fie
ld(u
V/cm
)
Core-1Core-2Core-3
Ic Criterion (1uV/cm)
-0.5
0
0.5
1
1.5
2
0 500 1000 1500 2000 2500 3000Current (A, DC)
Elec
trica
l Fie
ld(u
V/cm
)
Core-1Core-2Core-3
Ic Criterion (1uV/cm)
Sample: 3 meter 3-Core • Ic (Conductor) = Approx. 2660 – 2820A (DC, 77K, 1uV/cm)• Ic (Shield) = Approx. 2400 – 2500A (DC, 77K, 1uV/cm)
Conductor Shield
Very good match between test results and design values
YBCO Cable - Critical Current Measurement
9th Annual EPRI Superconductivity Conference – November 12, 2008
0.001
0.01
0.1
1
100 1000 10000Loading Current (Arms, 60Hz)
AC
loss
(W/m
/pha
se)
Measured value
Sample : 2.5 meter single coreCurrent loading : go & return through conductor and shieldMeasuring : Lock-in amplifier with electrical 4 terminals
0.34 W/m/ph @ 800 ArmsSlightly better result than the
1 meter test sample core
AC Loss Measurement
9th Annual EPRI Superconductivity Conference – November 12, 2008
Fault Current Test with 1 m 2G Sample CableFault Current Testing• Sample: BSCCO Core – YBCO Core
(Compare YBCO core with BSCCO one)• Current: 23kA• Duration: 8 – 38cycles• Cooling: Open Bath (77K)
Test Site : Nissin Electric (Kyoto)
0
10
20
30
40
50
60
70
80
90
100
0 10 20 30 40 50Duration [cycles, 60Hz]
Max
imum
Tem
pera
ture
Ris
e [K
]
BSCCO ConductorBSCCO ShieldYBCO ConductorYBCO Shield
Shield
Conductor
Generator(5000V)
Lg
L1 L2 L0Transformer(6600V/550V)
Test SamplesSWGenerator(5000V)
Lg
L1 L2 L0Transformer(6600V/550V)
Test SamplesSW
Temperature Rise During Faultnearly identical to BSCCO core
9th Annual EPRI Superconductivity Conference – November 12, 2008
Replacement of 30 meter section with new YBCO cable[ 30m cable Installation ]
[ Joint Re-assemble(BSCCO-YBCO)]
[ Termination Re-assemble ]
World first’s HTS cable replacement is completed!
9th Annual EPRI Superconductivity Conference – November 12, 2008
Summary of Various Commissioning Tests at Phase-II
100 kV, 5 minutes, each phase (based on AEIC) : good
350 m cable section (including joint): 1.0kWEntire cable system (not including CRS: 3.4kW
2.3kA (at 73K), 2.8kA (at 69K): Same Ic as Phase-I
Maximum core tension: approx. 1000kgTension minimized by “loosely stranded 3-core structure”
Vacuum level at each part: good (no leakage)Core behavior inside the joint: within the scope of Design
0.61 MPaG (based on ASME code): good
Test Results
DC withstand voltage test
Heat loss measurement(under no-load condition)
Ic measurement (dc, defined at 1uV/cm)
Initial cooling test
System withstand pressure Test
Test Items
HTS cable system successfully passed following commissioning tests:
-0.5
0
0.5
1
1.5
2
2.5
0 500 1000 1500 2000 2500 3000Current [A, DC]
Elec
tric
Fiel
d [u
V/cm
]Core-1
Core-2
Core-3
Ic critrion (1μV/cm)
Cable Mean Temp : 73K 69K
-200
-150
-100
-50
0
50
0 50 100 150 200 250 300 350 400
Length [m]
Tem
pera
ture
[]
SouthTermination
6H10H
18H1D 1.5D
10.5D11.5D
3D
9D
10.7D 10.8D 10.9D
0H
NorthTermination
0 50 100 150 200 250 300 350
9th Annual EPRI Superconductivity Conference – November 12, 2008
Demonstration of the world’s first device with 2G HTS wire in a live power grid
0
0.2
0.4
0.6
0.8
1
1.2
1/7 1/21 2/4 2/18 3/3 3/17 3/31
Date (2008)
Tem
pera
ture
Def
eren
ce [K
]
0
4
8
12
16
20
Tran
smitt
ed E
lect
ricity
[MVA
]
Temperature Deference between Outlet and Inlet of Cable
Transmitted Electricity
Cable made with 2G HTS wire was energized in the grid in January 2008 & performed without any issues
Jan 8 2008
9th Annual EPRI Superconductivity Conference – November 12, 2008
0
500
1000
1500
2000
2500
3000
3500
65 70 75 80Temperature [K]
Cri
tica
l Cur
rent
[A, a
t 1u
V/c
m]
Short Sample Ic(1800A at 77.3K)
Ic-T characteristicsof DI-BSCCO
0
500
1000
1500
2000
2500
3000
3500
65 70 75 80Temperature [K]
Cri
tica
l Cur
rent
[A, a
t 1u
V/c
m]
Short Sample Ic(1800A at 77.3K)
Ic-T characteristicsof DI-BSCCO
Commissiong Test(320m+30m Cable)
-0.5
0
0.5
1
1.5
2
2.5
0 500 1000 1500 2000 2500 3000Current [A]
Ele
ctri
cal F
ield
[uV
/cm
] Core-1Core-2Core-3
Ic criterion(1μV/cm)
73K69K
Variation of Critical Current from Phase-I through Phase-II
0
500
1000
1500
2000
2500
Sample Test Phase-I(after cooldown)
Phase-I(after long-term
operation)
Phase-II(after cooldown)
Phase-II(after long-term
opearion)
Cri
tica
l Cur
rent
[Adc
, at
73K
]
Core-1Core-2Core-3
• The Ic of long cable are very good match with expected value from short sample testing at 77K.
• The Ic values had no change through Phase-I and Phase-II including heat- cycles.
9th Annual EPRI Superconductivity Conference – November 12, 2008
Variation of Temperature Difference on the Cable during Phases I & II
0
0.2
0.4
0.6
0.8
1
1.2
7/20 8/17 9/14 10/12 11/9 12/7 1/4 2/1 3/1 3/29 4/26
Date (2006-2007)
Tem
pera
ture
Def
eren
ce [K
]
0
4
8
12
16
20
Tran
smitt
ed E
lect
ricity
[MVA
]
Temperature Deference between Cable Outlet and Inlet
Transmitted Electricity
[ Phase-I ]
0
0.2
0.4
0.6
0.8
1
1.2
1/7 1/21 2/4 2/18 3/3 3/17 3/31
Date (2008)Te
mpe
ratu
re D
efer
ence
[K]
0
4
8
12
16
20
Tran
smitt
ed E
lect
ricity
[MVA
]
Temperature Deference between Outlet and Inlet of Cable
Transmitted Electricity
[ Phase-II ]
• Temperature difference between outlet and inlet of the HTS cable was 0.9 +/- 0.1K• Temperature deference was very stable during the long-term In-grid operation in
Phase I and Phase II• Maintained good CRS operation and No change of cable heat loss during long-
term in-grid operation
9th Annual EPRI Superconductivity Conference – November 12, 2008
Presentation Summary
• World class team has successfully executed on all phases of the program– Met or exceeded all goals and objectives– Cable ran flawlessly for >12 months with ZERO instances of downtime due
to the HTS system– Efficient, reliable and robust design capable of handling ‘real-world’ utility
operating environment• ALL equipment/systems responded as designed without any adverse effects
– Biggest reliability concern (CRS) addressed & proven to meet commercial requirements
• Achieved World’s first in-grid demonstration of a YBCO device• Technology transfer & education achieved by numerous tours/events (>20) and
articles/presentations(>50) given throughout the program
9th Annual EPRI Superconductivity Conference – November 12, 2008
The Bottom Line…
“Of importance to National Grid is that this project has demonstrated the reliability of the technology. We encountered no difficulties in integrating the project into our grid and the entire installation was totally transparent to our customers. The system has stood up to very exacting utility standards and we look forward to further developments in HTS technology.”
- William Flaherty,Energy Solutions Regional
Director of National Grid
9th Annual EPRI Superconductivity Conference – November 12, 2008
Thank you!For more information:
www.superpower-inc.comor
12008년 12월 13일
Power System Network(345kV and above)
Power System Network(345kV and above)
345kV Overhead System
DC±180kV Cable Link
345kV Substation
Generating Plant
765kV Substation
765kV System
345kV Underground System
Legend
Classification 1999 2000 2001 2002 2003 2004 2005 2006 2007 2008Peak Demand 37,293 41,007 43,125 45,773 47,385 51,263 54,631 58,994 62,285 62,794Increase Rate 13.0 10.0 5.2 6.1 3.5 8.2 6.6 8.0 5.6 0.8
Peak Demand [MW]Peak Demand [MW]
Voltage 2008 2010 2014 2020
765kV 21.7 24.4 23.6 25.3
345kV 50.050.0 57.257.2 56.656.6 57.957.9
154kV 49.4 49.2 50.050.0 54.054.0
Transition of Fault Current [kA]Transition of Fault Current [kA]
The rate of underground transmission lineThe rate of underground transmission line
IncheonIncheon29.5%29.5%
SeoulSeoul51.3%51.3%
JejuJeju11.9%11.9%
DaejunDaejun45.2%45.2%
GwhangjuGwhangju26.5%26.5%
UlsanUlsan18.7%18.7%
BusanBusan31.5%31.5%
KangwonKangwon5.3%5.3%
JunbukJunbuk6.1%6.1%
KyungbukKyungbuk4.1%4.1%
KyunggiKyunggi18.3%18.3%
KyungnamKyungnam7.4%7.4%
ChungnamChungnam5.0%5.0% DaeguDaegu
21.9%21.9%
(As of 2007)
ChungbukChungbuk6.2%6.2%
Total12.68%
High Capacitance & Low loss + Eco-friendlyHTS Cable & SFCL
High cost for civil work and constructionDifficulty of excavating roads for construction of conduit or
culvertNIMBY for the construction of new substations in urban areaNeeds for environmental friendly power apparatusNeed to decide how to renewal the aged power cablesElectric power demand is increasing every year Continuous increase of fault current
• Project period : 2004~2011• Total budget : $146million(Government : $100million / Industry : $46million)• Participants
The name of Project : DAPAS The name of Project : DAPAS ((Development of Advanced power system by applied Superconductivity technology)
22.9kV HTS Cable has been developed and 22.9kV HTS Cable has been developed and 154kV HTS power cable is under development till 2010154kV HTS power cable is under development till 2010
2004 2005 2006 2007200320022001
1 ‘st Phase 2 nd Phase
FundamentalDesign
SingleCore 30m
50MVA/30m3-Core
50MVA/100m3-Core
Fab. Evaluation.
1,000MVA
2008 2009 2010
3 rd Phase
Evaluation Type test Demonstration on Real grid
Real-grid application
Design Fab. Evaluation Type test
DAPAS
Year
Basic study
154kV
22.9kV
Long termOperation
그림 1. MLI 개략도
MLI
Vaccum
Tcold= 77K
Thot= 300K
Spacer
Outer layer
Inner layer
0 500 1000 1500 2000 2500 3000 350050
100
150
200
250
300
350
1E-6
1E-5
1E-4
1E-3
0.01
0.1
1 Temperature
Tem
pera
ture
(K)
Time (hr)
Vacuum rate
Vac
uum
rate
(Tor
r)
HTS Cable
Cryostat
Fabrication
Experimental result
Displacement Simulation
Seamless Aluminum Cryostat for HTS Cable was developedSeamless Aluminum Cryostat for HTS Cable was developedFundamental Studies
Pitch determinationfor each layer Impedance matching
EM field calculation
Fabrication
HTS Shield
HTS Conductor
Optimal Design for Conductor/Shield Stranding & FabricationOptimal Design for Conductor/Shield Stranding & FabricationDesign & Fabrication of HTS Cable
HTS CableHTS Cable• Cold Dielectric• Diameter : 145mm• Seamless Aluminum Cryostat• PVC Sheath• ~ 35kV Insulation level• 3 - phases in one cryostat• FC Stabilizer incorporated
HTS Cable
• 22.9kV (Nominal), 13.2kV (Phase)• 1,260A (50MVA)
Fault Current : 25kA, 15cycle (Cu Stabilizer)Closed loop cryo-coolers incorporated in CRS
HTS Cable SystemHTS Cable System
Joint BoxJoint Box• Compact Design
(500mm Ø, 3.5m L)• ~ 35kV Insulation level • Pre-fabricated components• Pressure withstand : Min. 15bar
Cable coreCable Cryostat Bellows
Approx. 3500
Cable coreCable Cryostat Bellows
Approx. 3500Approx. 3500
Termination Termination • Compact Design
(800mm Ø, 3.5m L× 2.1m h)• ~ 35kV Insulation level • 3 - phases in one cryostat• Pressure withstand : Min. 15bar• Pre-fabricated components• Polymer composite Bushing
Approx. 3500
Appr
ox. 2
100
Insulator
BellowsCryostat
Approx. 3500
Appr
ox. 2
100
Insulator
BellowsCryostat
Design of Accessories
Pipe duct (175mm)Pipe duct (175mm)
TunnelTunnel
Snake and cleatsSnake and cleats(for TM behavior)(for TM behavior)
Installation & handling of HTS cable are same as ordinary cableInstallation & handling of HTS cable are same as ordinary cableInstalltion
PrePre--fabricated fabricated
••Jointing at site Jointing at site
TerminationTermination Joint BoxJoint Box
Minimum jointing work at site Minimum jointing work at site (14 days for termination, 21 days for joint box)(14 days for termination, 21 days for joint box)
PrePre--fabricated fabricated
Jointing Works
Configuration of CRS Configuration of CRS -- Closed loop ( no evaporation of LNClosed loop ( no evaporation of LN22 ) ) -- Total heat loss covered by packaged cryoTotal heat loss covered by packaged cryo--cooler cooler
GM840W@65K,
2EA
Separator
Sub-cooler
Ambient
HTS Cable & Acc.
Evaporator
Vacuum
Pump
Circulation
Pump
Heat
Exchanger
Pulse Tube
320W@65K
Stirling
Cryocooler
(640W @65K)
F
Coldbox1 Coldbox2
LN2Tank
(5 ton)
Bypass line
GM840W@65K,
2EA
Separator
Sub-cooler
Ambient
HTS Cable & Acc.
Evaporator
Vacuum
Pump
Circulation
Pump
Heat
Exchanger
Pulse Tube
320W@65K
Stirling
Cryocooler
(640W @65K)
F
Coldbox1 Coldbox2
LN2Tank
(5 ton)
Bypass line
CRS
Ground level
Joint box
Tunnel (55 m)
Pipe Duct [15 m]
Termination (Power source)Termination (Load)
Jointbox
U-bend
Termination (Load) Termination (Power source)
On the ground[30 m]
Configuration of system installation Configuration of system installation ( Fully simulating real grid conditions )( Fully simulating real grid conditions )
100 m
Evaluation
11stst Cool downCool down Reference Tests Load Cycle Test
•• Dielectric LossDielectric Loss•• Partial DischargePartial Discharge•• Dielectric securityDielectric security•• DC IcDC Ic
•• Applied Voltage Applied Voltage -- 1.5Uo for 30days1.5Uo for 30days
•• Load currentLoad current-- 1,260 A (8hrs On, 16hrs off)1,260 A (8hrs On, 16hrs off)
•• Cooling Circuit Pressure ControlCooling Circuit Pressure Control
•• DC Ic DC Ic •• PD (@Uo,1.5Uo, 2.5Uo)PD (@Uo,1.5Uo, 2.5Uo)•• Dielectric Loss (@Uo, 1.5Uo, 2.5Uo)Dielectric Loss (@Uo, 1.5Uo, 2.5Uo)•• Dielectric Security (@2.5Uo for 24h)Dielectric Security (@2.5Uo for 24h)••Thermal/Electrical loss (Ref.)Thermal/Electrical loss (Ref.)•• Impulse (BIL)Impulse (BIL)
Residual PerformanceTests
Warm-up & 2nd Cool down
•• Shrinkage (Ref.)Shrinkage (Ref.)
Test program Test program -- Reference tests for confirmation of sound installation Reference tests for confirmation of sound installation -- Main dielectric tests were executed after 2Main dielectric tests were executed after 2’’nd cool downnd cool down
Evaluation
Temperature profile during the whole type test procedureTemperature profile during the whole type test procedure
Referencetest
Residualtest
Test Results
Load Cycle Test at 1.5Uo for 30 days was successfully finishedLoad Cycle Test at 1.5Uo for 30 days was successfully finished
1 cycle
Time (h)
8h(1260A)
16h (No load)
Voltage
Current
(20kV ; 1.5U0)
Volta
ge &
Cur
rent
1 cycle
Time (h)
8h(1260A)
16h (No load)
Voltage
Current
(20kV ; 1.5U0)
Volta
ge &
Cur
rent
Test Results
* Background noise : 5~10 pC
PD, dielectric loss were tested successfullyPD, dielectric loss were tested successfully
Applied Voltage (kV) PD (pC) Tan δ
5 < 10 0.00002
10 < 10 0.000027
13.2 (Uo) < 10 0.000039
20.1 (1.5Uo) < 10 0.00004
33 (2.5Uo) < 10 0.000041
* High Frequency Antenna
Test Results
AC Dielectric Security Test @2.5Uo for 24hours was passed AC Dielectric Security Test @2.5Uo for 24hours was passed
Test Results
0 500 1,000 1,500 2,000 2,500 3,000 3,500
-2.0x10-3
0.0
2.0x10-3
4.0x10-3
6.0x10-3
8.0x10-3
1.0x10-2
1.2x10-2
1.4x10-2
1.6x10-2
Phase R @ 75K Phase S @ 75K Phase T @ 75K Phase R @ 72K Phase S @ 72K Phase T @ 72K
Ic criterion (1uV/cm)
Volta
ge (V
)
Current (A)
Phase(Cable)
Design @ 75 K
Result
75 K 72 K
R 3 kA 3.01 kA 3.34 kA
S 3 kA 3.06 kA 3.43 kA
T 3 kA 3.03 kA 3.34 kA
DC Ic showed no degradation after all electrical & thermal cycleDC Ic showed no degradation after all electrical & thermal cycle teststests
* Operating temperature : 72 ~ 75 K* Operating current range : ~ 1.8 kA
Operating range
Test Results
•• The 22.9kV 50MVA HTS cable system was developedThe 22.9kV 50MVA HTS cable system was developed
and successfully passed 3 and successfully passed 3 rdrd party inspected type testparty inspected type test
•• The proposed type test specification fully considers The proposed type test specification fully considers
the realthe real--grid operational conditionsgrid operational conditions
•• Long term verification in end userLong term verification in end user’’s reals real--grid has beengrid has been
planned for commercialization of HTS cable systemplanned for commercialization of HTS cable system
In 2008, the main topic of R&D on the HTS cable system is In 2008, the main topic of R&D on the HTS cable system is operation and maintenance skills regarding to the real grid operoperation and maintenance skills regarding to the real grid operationation
• History
• 2001 ~ 2003 : Fundamental studies • 2004 ~ 2005 : Application technologies • 2006 ~ 2007.6 : Type test for 22.9kV products
HTS Cable, Joint, Terminations, CRS
• Updated
• 2007.6 ~ 2008 : O&M Skills & 6 Times Thermal CyclesUnmanned operation Technology, Live line maintenance
• Planning
• 22.9kV 50MVA : Real grid application in KEPCO’s substationLonger than the length which needs joint box with network study
HTS Cable Updated
3phase 22.9kV/630A hybrid SFCL(2006)
Developed jointly by KEPRI and LS Industrial Systems.Combined Superconductor and normal-conductor devices.A 3φ 22.9 kV/630 A SFCL was built and tested for 3-phase faults
• Limited fault current 29 kA to 17 kA (and to 8 kA after 5 cycles)
A hybrid SFCLunder test
Cryostat Fast Switch Current Limiting Resistor
Control & Monitoring Parts
Last version of 3phase 22.9kV/630A hybrid SFCL(2008)
Field test of 22.9 kV Hybrid SFCL is planned in Gochang Testing Yard.Now, processing the network engineering
Superconducting power machine testing building
AutomaticFault generator
Reliability Test Plan
KEPCOHead Quarter
Prime Contractor
KEPCO(KEPRI)KERI
UniversityDetailed Feasibility
StudyOperating & Maintenance
Korea GovernmentKETEP
(Korea Institute of Energy and Resources Technology
Evaluation and Planning)
KEPCO(KEPRI)LS Cable
KERI, KBSiUniversity
Manufacture and Installation in HTS
Cable Systems
KEPCO(KEPRI)LS IS
UniversityManufacture and
Installation in SFCL Systems
• Project period : Nov. 2008 ~ Oct. 2013• Total budget : $17million
(Government : $8.5million/Industry : $8.5million)
154/22.9kV MTR
HTS Cable 500m
150MVA HTS Cables
3kA SFCL
[ 22.9kV HTS Cable, Termination, and Splice]
[ 22.9 kV SFCL System-Trial Product ]
Supplying the huge buildings with electric power by HTS cables
Replacing 22.9kV conventional cables(2~3lines) with the superconducting cables using the existing conduit or culverts without additional civil works
22.9 kVSW/S
22.9 kV Superconducting Cablesto replace 154 kV conventional cables
~
154 kV S/S in the suburbs
SFCL
SFCL
SFCL
22.9 kVSW/S
22.9 kV Superconducting Cablesto replace 22.9kV conventional cables
Superconducting Transformers
22.9 kVSW/S
Downtown Area
Circuit Breaker(Normal open)
Superconducting Power System (SPS) applying distributed switching stations for metropolitan areas
Apply superconducting power devices (cables, transformers, FCLs) to real power system154kV transmission power system 22.9kV superconducting power system
Replace 154kV substations in downtown with 22.9kV underground switching stationsReplace 154kV conventional cables with 22.9kV superconducting cablesBulk power transfer by superconducting cables and transformers & Fault current reduction by SFCL
Skip substations
Reduce construction costs
Environment-friendly
Avoid civil petitions
154kVS/S
154kVS/S
154kVS/S
154kVS/S
Downtown
154kV conventional cables
154kVS/S
154kVS/S
22.9kVSW/S
22.9kVSW/S
22.9kVSW/S
22.9kVSW/S
22.9kVSW/S
22.9kVSW/S
22.9 kVSuperconducting cables
Downtown
154kV conventional cables
Suburb Suburb
One of solutions for the site problemNo substations & Compact size Easy to find a site for power facilities in downtownUnderground switching stations Make a park on the switching stations
Economic benefitsReduction of cost for buying land
The site for 22.9kV switching stations is less than 30%, compared to 154kV substations.
No additional construction costWe can use established underground facilities such as existing electric power conduit pipes.
Environmental and social benefitsEnvironment-friendly Avoid the trend of NIMBY
No oil for cooling the systemFree of the explosion danger (Superconducting transformer)
No additional construction Reduce the construction cost and ease traffic congestionHigh efficiency and loss of superconductor Save energy and reduce CO2 emission
In Korean power system, increase of electric power demand have been accompanied with increase of power plants, substations, transmission lines and distribution lines. So that development of high capacitance power facility to accept increase demand was required and during a past decade, superconducting cable and SFCL have been developed.
Currently, developments and tests of 22.9kV superconducting cable and SFCL are finished, and development of 154kV superconducting system is under development till 2010.
From Nov.2008, to affirm stability and reliability of developed superconducting cable and SFCL by gathering and analysis of operating and maintenance data, 22.9kV HTS system real grid project is started for 5 years.
If stability of HTS system including superconducting cable and SFCL is affirmed, it will be expended from urban.
2008년 12월 13일 39
Southwire – Entergy HTS Cable Project
David KnollProject Manager
HTS Cable Systems
Eigth Annual EPRI Superconductivity ConferenceOak Ridge, TN
November 12-13, 2008
Erik GuillotProject Manager
Transmission EMCC
Project Partners
Project Specs
Cable Design HTS TriaxTM - SuperconductingLength 1760 meters (1.1 miles)Voltage 13.8 kVLoad 48 MVACooling Single Point, Closed CycleSplices 2 (Cable Sections = 3)In-Service Date 1Q2011
Cooling Plant13.8 kV, 2.0 kA (48 MVA) Triax HTS Cable
Project Location
Cable Route
Project Overview: Replace Copper HV Transmission with HTS MV Distribution
Problem:• Saturated 13 kV distribution – anticipate high load growth• 230/13 subs to north & south of area - Need new sub at mid-point
Challenges:• OH RoW for 230 or 13 kV very difficult or impossible• Small footprint available for new substation• 230 kV solution: placing transformer in dense residential area.• 13 kV conventional: Voltage drop, power quality
Solution:• 13 kV HTS cable to transmit 48 MVA into small footprint station.• 1.1 mile HTS cable that meets load growth needs.• Leverage existing transformer capacity – No new transformers needed• Single point cooling station.• 13 kV HTS replaces 230 kV underground.• Cost effective with DOE support.
Southwire - HTS TriaxTM 2000A Cable
CryostatFormer Phase 1 HTS
Phase 2 HTS
Dielectric
Phase 3 HTS
Copper Neutral
LN
LN
HTS TriaxTM Advantage vs Competition:1. ½ HTS tape usage = substantially cheaper2. Single Cable = simplified mfg & installation3. Smaller cold surface area = lower cooling & operating cost
Southwire Triax Cable Termination
3 Phase Connections
Neutral Connection
- Provides transition from superconducting materials to copper materials.
- Thermal transition from –200 C to ambient temperature
- Controls electrical stresses.
- Provides input and/or output location for LN coolant.
- Provisions made for temperature and pressure measurements and monitoring.
- Electrical connections to utility made by means of industry standard NEMA pad.
Cable Installation
On Going Effort - HTS Tape Options
• 1G BSCCO vs 2G YBCO– Mechanical testing– Compatibility with cabling process– Electrical Properties – Ic, n-Value, AC Loss– Magnetic Properties– Piece Lengths– Wire availability– Per meter costs
On Going Effort – Cable Configuration
1G 2GComposite 1 1G
Segment 1 Segment 2 Segment 3 Spare
1G 2G2G 1G
1G 1G
2G2G
1G
1G 1G
2G 2G
Composite 2
All 1G
All 2G
On Going – Thermal / Hydraulic Analysis
Former, RT
Heater - Qknown
Insulation – RT
Heater - Qknown
Insulation – RT
Heater - Qknown
Insulation – RT
Cryostat WallLN2
LN2
Temp Sensors
THERMAL MODEL
Former, RT
HTS – AC Loss, RT
Insulation – RT
HTS – AC Loss, RT
Insulation – RT
HTS – AC Loss, RT
Insulation – RT
Cryostat WallLN2
LN2
CABLE ASSEMBLY
66
67
68
69
70
71
72
73
74
0 500 1000 1500 2000L [m]
T [K
]
AnnulusFormerTmaxPh1Ph2Ph3Neutral
On Going Effort – Cryogenic System Design
• ~ 10kW cooling required
• Closed loop cooling system
• Cryocooler Options– Pulse Tube– Sterling Cycle– Brayton Cycle
• RFP’s out after AC Loss study
• System supplier will perform detailed system design
Heat ExchangerClosed Cycle
n…
HTS Cable
Back-upOpen Cycle
21
Cryocooler Bank
LN2Tank
Sub-Cooled LN2Counter Flow Cooling
Out = thru formerIn = thru annulus
Previous Experience – AEP, Columbus, OH
AEP-Bixby200 meters8/2006 to present13.2 kV, 3.0 kA,Triax Cable
5 DAY Bixby Peak Load – August 2007
Peak Load = 2,715 A
0
500
1000
1500
2000
2500
3000
0:00:00 0:00:00 0:00:00 0:00:00 0:00:00
Cur
rent
(Am
ps)
Phase 1
Phase 2
Phase 3
Neutral
AEP Data – Fault Currents
07/11/200801:24:20.500
07/11/200801:24:27.425
No measurable thermal response in HTS cable or terminations.
• Transient event: I ≥ 3.0 kA (2,121 A-rms)
• 74 total events– 39 events with >4,242 A-pk (3,000 A-rms)– 19 events with >5,657 A-pk (4,000 A-rms)– 13 events with >7,071 A-pk (5,000 A-rms)– 7 events with >14,142 A-pk (10,000 A-rms)– Highest current = 17,765 Apk (222
milliseconds)– Longest duration = 1.785 seconds (5209
Apk, 3683 Arms)
• HTS cable never taken out of service.
1 /31
“ Evaluation of 100m long 22.9kV 50MVA HTS Cable System”
S. K. LEEPrincipal Research EngineerElectric Power R&D CenterLS Cable Ltd
EPRI Superconductivity Conference
Development status up to 154kVDevelopment status up to 154kVHTS Cable Systems in KoreaHTS Cable Systems in Korea
12 Nov. 200812 Nov. 2008
KEPRI (KEPCO)KEPRI (KEPCO)ByeongByeong--Mo YangMo Yang
2 /31
Contents
About DAPAS program
• R&D Results of HTS cable in 1st & 2nd Phase
• Plan of 3 rd Phase
• Conclusion
3 /31
DAPAS program
DAPAS program
• Development of Advanced Power system by Applied Superconductivity tech.• Name of the “superconductivity frontier program in Korea”• Selected on May. 2001 by MOST• Funded about 100 million US dollars for ten years from government.
The primary target
• R & D and commercialization of the developed HTS products
Budget
10 years(2001~2010) 148 million $ ( Gov. : 100 & Ind. : 48 )
2007. 04 - 2008. 03 14 million $ ( Gov. : 10 & Ind. : 4 )
4 /31
Development targets for each phase
FY
Phase
Target
2001 2002 2003
1st Phase
Core technology(to develop the HTS wire and system technology)
2004 2005 2006
2nd Phase
Pre-commercial pilot(to improve the 1st
phase technology and develop the prototype devices)
2007 2008 2009 2010
3rd Phase
Commercialization(Field test and development of the industrial technology for commercialization)
Power cables
50MVA, 22.9kV cable
50MVA, 22.9kV, 100m system
1GVA, 154kV, 3 phase
Transformers
Fault-current limiters
Motors
1MVA, 22.9kV Single phase
6.6kV, 200Arms SFCL
100~ hpmotor
core technologies
22.9kV, 630Arms SFCL
1MVA~motor
33MVA, 154kV Single phase
22.9kV, 3kA & 154kV, 4kArms
5MVAmotor
5 /31
30m 100m 200m 350m 500m
50m 120m
36kV
66kV
138kV
154kV
225kV
NKT (~02)
SEI (~99)
SEI & TEPCO (~01)
24kVPirelli, AMSC,
DTE (~01)12.5kV
S’wire & IGC (~00)
620m
34.5kV
77kVFurukawa (~04)
22.9kV
250m
3 phase, 1 cryo, CD Succeeded DAPAS Warm Dielectric 1G wire3 phase, 3 core, CD Failed Cold Dielectric 2G wire3 phase, 3 core, WD1 phase, CD 1 core 3 ph
DAPAS(~04)
(~07)
DAPAS (~11) LIPAAMSC&Nexans
LIPA (~07)
Albany
AEP
S’wire & NKTAMSC (~07)
IGC & SEI (~07)
1,780m
13.8kV
S’wire &NKT(~11)
SPE project
SPELIPA 2
AMSC&NexansLIPA (~11)
SEI&TEPCO(~11)
Highest voltage class
6 /31
History of HTS power cable in DAPAS
5m Cable core + 10m Cooling System
30m Single Phase HTS Cable System22.9kV, 50MVA
30m Three Phase HTS Cable System22.9kV, 50MVA
2001 2003 2005Aug., 2005Long Term Test
7 /31
Termination (Load)Termination (Load)
Ground levelGround level
Joint boxJoint box
Termination (Load)Termination (Load) Termination (Power source)Termination (Power source)
Tunnel (55 m)Tunnel (55 m)
Pipe Duct [15 m]Pipe Duct [15 m]
Termination (Power source)Termination (Power source)
JointJointboxbox
UU--bendbend
On the groundOn the ground[30 m][30 m]
Fully simulating real grid conditions
HTS Cable in KEPCO Testing Center in 2006
8 /31
Specification
• Voltage : 22.9kV (Nominal), 13.2kV(Phase)
• Current : 1,260A (50MVA)
• Fault Current : 25kA, 15cycle
• Cryogenic system : Closed loop cryo-coolers
• Cable length : 100m
Cable
Approx. 3500
Appr
ox. 2
100
Insulator
BellowsCryostat
Approx. 3500
Appr
ox. 2
100
Insulator
BellowsCryostat
Termination Joint Box
Cable coreCable Cryostat Bellows
Approx. 3500
Cable coreCable Cryostat Bellows
Approx. 3500Approx. 3500
9 /31
Pipe duct (175mm)
TunnelTunnel
Snake and cleatsSnake and cleats
Installation & handling of HTS cable are same as ordinary cable
Installation
10 /31
• Specification of type-test - Optimal test items & conditions - Suitable to real grid application
Proposed to IEC SB1 by LS Cable ( under discussing )
• Certification by 3rd party test institute- Kinetrics, Canada
• Confirmation by end user- KEPCO/KEPRI- Gochang power testing center
Evaluation
11 /31
Load Cycle Test at 1.5Uo for 30 days was successfully finished
1 cycle
Time (h)
8h(1260A)
16h (No load)
Voltage
Current
(20kV ; 1.5U0)
Volta
ge &
Cur
rent
1 cycle
Time (h)
8h(1260A)
16h (No load)
Voltage
Current
(20kV ; 1.5U0)
Volta
ge &
Cur
rent
Test Results (I)
PD and dielectric loss were tested successfully
* Background noise : 5~10 pC
Applied Voltage (kV) PD (pC) Tan δ
5 < 10 0.00002
10 < 10 0.000027
13.2 (Uo) < 10 0.000039
20.1 (1.5Uo) < 10 0.00004
33 (2.5Uo) < 10 0.000041
* High Frequency Antenna
12 /31
AC Dielectric Security Test @2.5Uo for 24hours was passed
Test Results (II)
No degradation after all electrical & thermal cycle tests
0 500 1,000 1,500 2,000 2,500 3,000 3,500
-2.0x10-3
0 . 0
2 . 0 x 1 0-3
4 . 0 x 1 0-3
6 . 0 x 1 0-3
8 . 0 x 1 0-3
1 . 0 x 1 0-2
1 . 2 x 1 0-2
1 . 4 x 1 0-2
1 . 6 x 1 0-2
P ha se R @ 7 5 K P ha se S @ 7 5 K P ha se T @ 7 5K P ha se R @ 7 2 K P ha se S @ 7 2 K P ha se T @ 7 2K
Ic criterion (1uV/cm )
Volta
ge (V
)
C u rren t (A )
Operating range Phase(Cable)
Design @ 75 K
Result
75 K 72 K
R 3 kA 3.01 kA 3.34 kA
S 3 kA 3.06 kA 3.43 kA
T 3 kA 3.03 kA 3.34 kA
* Operating temperature : 72 ~ 75 K* Operating current range : ~ 1.8 kA
13 /31
AC Loss was measured by calorimetric method on site
AC Loss
Loss (W)
W/m.phase @ 1260ArmsDesign Measured
Heat Loss AC loss Total Heat Loss AC loss Total
Cable
70m 165.0 210.0 375.0 164.8 255.2 420.0 AC loss : 1.21 W/m∙phase
30m (U-band)
105.0 90.0 195.0 102.9 113.2 216.1 AC loss : 1.25 W/m∙phase
Termination 165.0 135.0 300.0 180.0 157.6 337.6
• 0.8W/m·phase @ 1260Arms in the Lab
14 /31
Plan (the 3rd phase)
15 /31
Target of 3rd phase (2007 ~ 2011)
R&D of 154kV, 1 GVA HTS Cable
- Specification : 154kV, 1GVA, 3phase, 100m
- Install the Power Grid in KEPCO Testing Center
154kV 2000SQ 154kV 2000SQ XLPE 2 LIneXLPE 2 LIne
154kV Over Head Line154kV Over Head Line(Youngkwang Nuclear Plant))(Youngkwang Nuclear Plant))
300m300m
TunnelTunnel
100m100m
Substation at GochangSubstation at Gochang
154kV HTS Cable will be installed in 2010
16 /31
25621
35851
24577
32996
27320
37293
30327
41007
32559
43125
34985
45773
36809
47385
39057
51246
41625
54631
43513
58994
0
10000
20000
30000
40000
50000
60000
70000
Capa
cita (
MW
)
1997 1998 1999 2000 2001 2002 2003 2004 2005 2006
Year
Peak loadAverage load
Peak and average load for a year
After 1997 financial crisis in Korea
Last year 2007, over
60GW
17 /31 17
Status and Analysis of KEPCO Grid
SeoulRegion
42%
East Region7%
Middle Region
13%
South-WestRegion
8%
South-East Region
30%
1) Regional Load : Highest Seoul Region (42%)
2) Underground Cable among T/L : Highest Seoul Region (73.9%)
3) Increasing Underground T/L : about 12.68% (the rate of Underground T/L in Korea)
VoltageVoltage T/L LengthT/L Length Rate(%)Rate(%)
345kV345kV 9393 77
154kV154kV 1,1431,143 9292
66kV66kV 1313 11
단위 :C-Km
Necessity of Transmission HTS Cable in KEPCO
IncheonIncheon29.5%29.5%
SeoulSeoul51.3%51.3%
JejuJeju11.911.9%%
DaejunDaejun45.2%45.2%
GwhangjuGwhangju26.5%26.5%
UlsanUlsan18.7%18.7%
BusanBusan31.5%31.5%
KangwonKangwon5.3%5.3%
JunbukJunbuk6.1%6.1%
KyungbukKyungbuk4.1%4.1%
KyunggiKyunggi18.3%18.3%
KyungnamKyungnam7.4%7.4%
ChungnamChungnam5.0%5.0% DaeguDaegu
21.9%21.9%
(As of 2007)
ChungbukChungbuk6.2%6.2%
Total12.68%
18 /31 18
Necessity of Transmission HTS Cable in KEPCO
HTSSuperconductor
LN2
150 mmHTS SC Cable
(154kV, 3.75kA, 1cct)800 mm
OF Cable (345kV, 840A, 2cct)
Cu Conductor150mm
19 /31 19
Applying Scenario of Transmission HTS Cable
154kV Overhead Line
:Suburbs Large City
154kV Conventional Cable
154kV HTS Cable
: Center of Large City, high load density
345kV Substation
Considerable Places for Applying HTS Cable to KEPCO Grid
Replacement from Old Conventional Cable
Construction of New T/L in Large City
Enlargement of T/L due to increasing load in Large City
Applying Concept of Transmission HTS Cable in KEPCO
20 /31
C
A B
Ia
IbIc
ISa
ISb ISc
15kA3kA 12kA9kA6kA
Fault Analysis of 154kV HTS Cable by Using EMTDCFault Analysis of 154kV HTS Cable by Using EMTDC
Modeling of Transmission HTS Cable in KEPCO
21 /31
HTS Phase ConductorHTS Phase Conductor
Outer CryostatOuter Cryostat
Former/StabilizerFormer/Stabilizer
InsulationInsulation
HTS ShieldHTS Shield
LN2LN2
Inner CryostatInner Cryostat
Thermal InsulationThermal Insulation(MLI + Vacuum)(MLI + Vacuum)
• Electrical Characteristics
- Rated Voltage : 154 kV
(U0, Um = 89, 170 kV)
- Rated Current : 3.75 kA
- BIL : 750 kV
- Design Fault Current
: 50 kA, 1.7s
• Physical Characteristics
- Cold Dielectric Design
(Single Phase in One Cryostat)
Design of 154kV/1GVA HTS Cable
154 kV, 1GVA HTS Cable Cross Section 154 kV, 1GVA HTS Cable Cross Section
22 /31
154kV/1GVA Stabilizer Design
-Fault Condition : 50 KA/ 1.7s
15.5 cycle10.5 cycle
5.5 cycle
Stabilizer Size Min. 610 mm2
Temp. Limit : 94 K (5 bar)Initial Temp. : 77 K
Core Design for 154kV/1GVA HTS Cable
23 /31
HTS Wire Evaluation for Cable Application
The Mechanical & Thermal Properties of multi-kinds of HTS wires evaluated
Multi-BendingTential Stress
Thermal Cycling & Twisting
24 /31
Insulation Design of 154kV HTS Cable
Breakdown s trength [kV/mm]
Bre
akd
ow
n w
eib
ull p
rob
ab
ility [
%]
757065605550454035
99
90
8070605040
30
20
10
5
3
2
1
0.1
25.18 68.39 15 0.633 0.088
26.39 61.65 15 0.310 >0.250
20.19 55.76 15 0.431 >0.250
Shape Scale N AD P
100
125
170
Variable
y = 40.043x-0.0514
y = 40.175x-0.0235
y = 51.097x-0.0336
0
5
10
15
20
25
30
35
40
45
50
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05 1.E+06T ime [s e c ]
Bre
akd
ow
n v
olt
ag
e [
kV
]
11
100 125 170
Breakdown s trength [kV/mm]
Bre
akd
ow
n w
eib
ull p
rob
ab
ility [
%]
13012011010090807065
99
90
8070605040
30
20
10
5
3
2
1
0.1
16.10 120.6 15 0.540 0.164
17.47 110.8 15 0.543 0.160
17.64 100.9 15 1.092 <0.010
Shape Scale N AD P
100
125
170
Variable
• PPLP for EHV application
• Insulation Thickness
< 15mmt
• Overall Diameter < 145mm
AC Weibull Test
AC V-t Test
Impulse Weibull Test
25 /31
DC 15,000 Amp / 5V
[ DC power supply ][ Cryogenic Vessel for Variable Temp.]
Cryogenic Characteristic Test of 154kV/1GVA HTS Cable
66K~77K, 5bar
26 /31
Termination of 154kV/1GVA HTS Cable
27 /31
5600W @ 65K
Phase APhase A
Phase BPhase B
Phase CPhase C
CryoCryo--CoolerCoolerLNLN22
StorageStorage
LN2 FlowLN2 Flow
Cryogenic System of 154kV/1GVA HTS Cable
28 /31
Place : Gochang Testing Center
Design : 2007.11
Start : 2008.3
Finish : 2009.9
Testing Facility for HTS Cable by KEPCO
154kV Superconducting Cable Test will be start 2009.6
29 /31
PQ시험장 OF케이블시험장
GIL시험장
교량첨가시험장
열거동시험장
시료설치용
전력구
배선용전력구
초전도시험장
HTS Cable Test Field (Tunnel)
Testing Facility Design
30 /31
2008. 6. 9 Berlin Germany11th IEC TC90 Meeting,
Proposed the Test Procedure the HTS Cable, like as Ic Measurement Procedure.Suggest the round robin test the HTS cable for standard
Status of Standard for HTS cable
2008. 8. 27, Paris FranceCIGRE SCD1 Working Group Meeting WG.15(Superconducting and Insulating Materials for HTS Power Applications)
Proposal the Specification of HTS ApplicationProposals for test procedures of HTS power equipment and electrical insulation.
CIGRE SC B1 (Insulated Cable) Decide to make TF for studying the specification of HTS cable
Korea The KS (Korean Standard) is in progress for “Ic Measurement Procedure of HTS Cable”
31 /31
Conclusion
• The 22.9kV 50MVA HTS cable system was developed
and evaluated
• 154 kV , 1GVA HTS cable system is being developed in the 3rd
Phase of DAPAS program
< 21/21 >
• HTS Cable R&D is moving from Grid Test to Grid Use in the world
• Suggestion on the Collaboration for studying
Standard of HTS Cable Testing Procedures
32 /31 < 21/21 >
superior performance.powerful technology.
SuperPower, Inc. is a subsidiary of Royal Philips Electronics N.V.
Status of 2G HTS Wire Technology Development and Manufacturing at SuperPower
Chuck WeberY.-Y. Xie, Y. Chen, X. Xiong, K. Lenseth, M. Marchevsky, A. Rar, Y. Qiao, B. Gogia, A. Knoll, R. Schmidt, D. Hazelton, and V. Selvamanickam
EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Funded by Title III Program, DOE and AFRLSupported by CRADAs with Los Alamos, Oak Ridge, & Argonne National Laboratories
2EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
SuperPower’s 2G wire is based on high throughput processes & superior substrate
YBCO
LaMnO3
MgO (IBAD + Epi layer)
Al2O3
100 nm
Y2O3
Hastelloy C-276
YBCO
LaMnO3
MgO (IBAD + Epi layer)
Al2O3
100 nm100 nm100 nm
Y2O3
Hastelloy C-276
2 μm Ag
20μm Cu
20μm Cu50μm Hastelloy substrate
1 μm YBCO - HTS (epitaxial)~ 30 nm LMO (epitaxial)
~ 30 nm Homo-epi MgO (epitaxial)~ 10 nm IBAD MgO
< 0.1 mm
• High throughput is critical for low cost 2G wire and to minimize capital investment• SuperPower’s 2G wire is based on high throughput IBAD MgO and MOCVD
processes• Use of IBAD as buffer template provides the choice of any substrate• Advantages of IBAD are high strength, low ac loss (non-magnetic, high resistive
substrates) and high engineering current density (ultra-thin substrates)
3EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
SuperPower’s 2G pilot manufacturing facility has been operational since 2006
Pilot IBAD
Pilot Substrate Electropolishing
Pilot buffer Sputtering
Pilot MOCVD
• Majority of investment already made for 1000 km/year capability
4EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Our main objective in 2008 was to meet market requirements for 2G wire• Replace 1G wire in large HTS device demonstration projects in the
U.S. and around the world– Key requirements: Long length, availability, Ic, price
• Supply large volumes of 2G wire to customers who have been waiting to take advantage of the superior performance of 2G
– Key requirements: Long length, Ic, additional performance metrics such as in-field Ic, ac losses, joints, insulation, FCL metrics …
• Advance towards medium-term goal of replacing copper wire in commercial HTS projects and challenge LTS wire in high-field applications
– Key requirements: Long length, availability, Ic, price, in-field performance and other additional performance metrics
5EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
High current metric: Capability of ~ 1000 A in 12 mm widths achieved!
2005 SmYBCO
2006 SmYBCO
2007 GdYBCO
0
1
2
3
4
5
6
7
0 1 2 3 4
Thickness (μm)
Jc (M
A/c
m2 )
2008 (GdY)BCO
3.3 μm film made in 10 passes: Ic = 976 A = 833 A/cm (Jc = 2.44 MA/cm2)2.1 μm film made in 6 passes: Ic = 929 A = 774 A/cm (Jc = 3.68 MA/cm2)
All achievements using production buffer tapes
Ic measurement using continuous dc current (no pulsed current) across entire tape width of 12 mm. No patterning
Over 1+ m length,Ic = 976 A = 813 A/cm
2008 (GdY)BCO
2005 SmYBCO
2006 SmYBCO
2007 GdYBCO
0100200300400500600700800900
0 1 2 3 4Thickness (μm)
Criti
cal c
urre
nt (A
/cm
-wid
th)
6EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
High current technology is being transferred to pilot MOCVD
0 5 10 15 20 25 30 35 40 45 50 550
100
200
300
400
500
Ic (A
/cm
-w)
Position (m)
Minimum Ic > 400 A/cm-w over 55 m length
Over 55 m length,
Minimum Ic = 481 A = 401 A/cm
At 0.2 μV/cm voltage criterion
All achievements using production buffer tapes. MOCVD process speed 90 m/h (4mm equivalent)
Over 10 m length,
Ic = 481 A = 401 A/cm
At 0.1 μV/cm voltage criterion
-1.0E-07
0.0E+00
1.0E-07
2.0E-07
3.0E-07
4.0E-07
5.0E-07
0 100 200 300 400 500
Current (A/cm-w)
Volta
ge (V
/cm
)
Ic = 450 A/cm-w at 0.1 μV/cm voltage criterion
7EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
In-field performance metric: dramatic improvements achieved by Zr doping
BZO additions have been very effective in improving in-field performance of PLD films, but was yet to be demonstrated with MOCVD.
Gd substitution results in strong pinning parallel to the tape.Zr doping strongly enhances pinning perpendicular to tape & in intermediate fields2 to 2.5x improvement in Ic by Zr doping. Thin films and thick films
020
4060
80100
120140
160180
-20 0 20 40 60 80 100 120
Angle between field and tape (deg)
Ic (A
/cm
)
0.7 micron SmYBCO
0.7 micron GdYBCO
0.7 micron Zr:GdYBCO
77K, 1T 77K, 1 T0
50100150200250300350400450
-20 0 20 40 60 80 100 120
Angle between field and tape (degrees)Ic
(A/c
m)
3.5 micron SmYBCO2.8 micron GdYBCO
3.3 micron Zr:GdYBCO
Data from Y. Zhang, M. Paranthaman, A. Goyal, ORNL
186 A/cm
229 A/cm
8EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Excellent in-field performance at 65 K, 3 T
150
200
250
300
350
400
450
500
550
-20 0 20 40 60 80 100 120Angle (deg)
• Title III Phase 3 program goal is Je without stabilizer of 15,000 A/cm2 at 65 K, 3 T
• Minimum Ic = 267 A/cm corresponds to Je of 41,000 A/cm2 at 65 K, 3 T
• Ic perpendicular to tape = 340 A/cm corresponds to Je of 52,300 A/cm2
2007: 2.8 μm(Y,Gd)BCO
2008: 3.15 μmZr:(Y,Gd)BCO
2008: 3.33 μmZr:(Y,Gd)BCO
160 A/cm
181 A/cm
2007 (Gd,Y)BCO
67%267 A/cmMinimum Ic
88%340 A/cmB // c
Improvement2008 Zr-doped (Gd,Y)BCOIc (77 K, 1 T)
Data from Y. Zhang, M. Paranthaman, A. Goyal, ORNL
9EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Zr-doped chemistry has been successfully transferred from Research system to Pilot MOCVD
0102030405060708090
100110120130140150160
-20 0 20 40 60 80 100 120 140 160 180Angle between magnetic field & tape (degrees)
Crt
ical
cur
rent
(A)
(Y,Sm)BCO(Y,Gd)BCO(Y,Sm)BCO with Zr(Y,Gd)BCO with Zr
Data from Y. Zhang, M. Paranthaman, A. Goyal, ORNL
Long-length wires are now being produced with Zr-doped chemistry
10EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
In 2007, we demonstrated world record high-field magnet
SuperPower coil tested in NHMFL’s unique, 19-tesla, 20-centimeter wide-bore, 20-megawatt Bitter magnet
05
1015202530
0 50 100 150 200 250
Current (A)
Cen
tral
Fie
ld (T
)
19T background self field
26.8 T @ 175 A
9.81 T @ 221 A
78 A in 4 mm width (77 K, self field)
Average Ic of wires in coil
~ 462 m2G wire used
12 (6 x double)# of Pancakes
~ 87 mmWinding OD
19.1 mmWinding ID
9.5 mm (clear)Coil ID
Coil tested by H. Weijers, D. Markewicz, & D. Larbalestier, NHMFL, FSU
0.73 T generated by coil at 77 K
11EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
New coil in 2008 with Zr-doped (Gd,Y)BCO wire with better in-field performance
~ 44.4
~1.569
~ 2772
~ 462
6
~ 51.6
~ 87
19.1
9.5
2007 coil
2008 coil
~1.635Coil Je (A/mm2) per amp of operating current
~ 2664# of turns
~ 41.9Coil constant (mT/A)
~ 4802G tape used (m)
6# of double pancakes
~ 56.7Coil Height (mm)
~ 87Winding OD (mm)
28.6Winding ID (mm)
21Coil ID (mm) clear 72 to 9772 – 82Wire Ic (A) 4 mm
2008 coil2007 coil
12EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
30% higher field in 2008 coil made with wire with improved in-field performance
0
5
10
15
20
25
30
35
-20 0 20 40 60 80 100 120 140 160
Angle between field and wire (degrees)
Ic (A
) for
4 m
m w
ide
wire
(Y,Sm)BCO wire 2007 coil(Y,Sm)BCO wire 2007 coilZr:(Gd,Y)BCO wire for 2008 coilZr:(Gd,Y)BCO wire for 2008 coil
77 K, 1 T (ORNL)
75 K, 0.92 T (LANL)
Temperature Coil current
Max Central Field
(K) (A) (T)77.4 22.7 0.95
70.25 44 1.8465.8 54 2.2664.5 57 2.3963.8 58 2.43
0.73 T
2007 coil with (Y,Sm)BCO
2.39 T65 K
30%0.95 T77 K
Improvement2008 coil with Zr-doped (Gd,Y)BCO
Temperature
13EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
This improvement remains effective at low T
0.75
1.00
1.25
1.50
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
B[Tesla] at 30o w.r.t. the tape surface
[Ic/Ic
@ 7
7K 0
T- 2
008]
/[Ic/
Ic@
77K
0T-
2007
] 60 K50 K40 K30 K20 K
Measurement done by M. Ogata and K. Nagashima at Railway Technical Research Institute
20-35% improvement in magnetic field range up to 4T
T =
14EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Continued routine manufacturing of kilometer lengths of fully buffered tape in CY 2008
4
5
6
7
8
0 200 400 600 800 1000 1200 1400 1600Tape position (m)
In-p
lane
text
ure
(deg
rees
)
12 tapes with complete 5-layer buffer stack, by ISS2007, and now over40 tapes have been produced in lengths of 1,300 m to 1,500 with in-plane texture of 5 – 7 degrees and excellent uniformity of ~2%
Manufacture of kilometer-lengths of high quality, fully-buffered tape was routine throughout 1 year
15EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Challenges in fabrication of complete, kilometer long 2G wire
Kilometer lengths limited by a few bad regions in an otherwise uniform wire;Major sources of the problems identified:
– MOCVD instability;– Mechanical damage;– Substrate defects
0
50
100
150
200
250
0 200 400 600 800 1000
Position (m)
Ic (A
/cm
)
050
100150200250
0 200 400 600 800 1000Position (m)
Ic (A
/cm
)
0
100
200
300
400
0 200 400 600 800 1000Position (m)
Ic (A
/cm
)
16EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Aug. 2008: Yet another world record!
0
50
100
150
200
250
300
350
400
450
0 200 400 600 800 1000
Position (m)
Ic (A
/cm
)
77 K, Ic measured every 5 m using continuous dc currents over entire tape width of 12 mm (not slit)
Voltage criterion = 0.2 microvolt/cm
Except for three spots, Ic of rest of 1,030 m > 300 A/cm 4mm: 120 A
200 mIc > 350 A/cm4 mm: 140 A
320 mIc > 350 A/cm4 mm: 140 A
310 mIc > 350 A/cm4 mm: 140 A
233,8102271030190,260302630181,980337540
Ic × Length (A-m)Minimum Ic (A/cm) @ 0.2 μV/cmLength (m)
17EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Aug. 2008: Ic > 300 A/cm achieved over 600 m
190,260302630181,980337540
Ic × Length (A-m)Minimum Ic (A/cm) (0.2 μV/cm)
Length (m)
0
50
100
150
200
250
300
350
400
450
0 100 200 300 400 500 600
Position (m)
Ic (A
/cm
)
77 K, Ic measured every 5 m using continuous dc currents over entire tape width of 12 mm (not slit)
Voltage criterion = 0.2 microvolt/cm Except for four spots, Ic of rest of 630 m > 350 A/cm
18EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
10
100
1,000
10,000
100,000
1,000,000
May
-02
Oct
-02
Mar
-03
Aug
-03
Jan-
04Ju
n-04
Nov
-04
Apr
-05
Sep
-05
Feb-
06Ju
l-06
Nov
-06
Apr
-07
Sep
-07
Feb-
08Ju
l-08
Crit
ical
Cur
rent
* Le
ngth
(A-m
)
Remarkable progress in 2G HTS wire scale-up over the last 6 years
0
40,000
80,000
120,000
160,000
200,000
240,000
Nov
-01
Jul-0
2
Mar
-03
Nov
-03
Aug
-04
Apr
-05
Dec
-05
Aug
-06
Apr
-07
Jan-
08
Sep
-08
Crit
ical
Cur
rent
* Le
ngth
(A-m
)
62 m18 m1 m 97 m
206 m
1 m to 1,300 m in 6 years
158 m
322 m427 m
595 m
World Records
790 m
1,311 m
935 m
Growth in last year
19EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Great strides made in 2008 in all key metrics
30%0.950.73Coil: Field at 77 K (T)
212%630202103Length with Ic > 300 A/cm (m)
98%337170Ic over 500 m (A/cm)
88%340181Ic (A/cm) at 65 K, 3 T
97%229116Ic (A/cm) at 77 K, 1 T
220%1030322322Length with Ic > 200 A/cm (m)
39%40651002G Wire Price ($/m)
233,810
1,311
378*
813
ISS 2008
120%595322Completed 2G wire Piece Length (m)
37%595470Ic (A/cm) over 1 m
102,935
227*
ISS 2007
127%
67%
Improvementin past year
246Ic over 200 m (A/cm)
70,520Ic × L (A-m)
ISS 2006Metric
*at 100 to 200% higher speed than in 2006
20EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
0
20
40
60
80
100
120
140
160
180
0 100 200 300 400 500 600 700 800 900 1000 1100 1200Position (m)
Ic (A
)Location of joints
Per customer’s requirement, 1200 m long wire was produced with 11 splices in a production operation. Arrangement of the 12 segments along the length was decided based on communication with customer so that the Ic profile would fit the coil winding requirements
Development of Practical Conductors - Joints
21EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Excellent resistance measured in all joints and mechanical robustness also demonstrated
All but one of the joints showed resistance around 33 nΩ, One joint showed a resistance of 100 nΩ, still within limit
-1.00E-05
0.00E+00
1.00E-05
2.00E-05
3.00E-05
4.00E-05
5.00E-05
6.00E-05
0 20 40 60 80 100 120 140
Current (A)
Volta
ge (V
olt)
Joint#1: 70-75mJoint#2: 175-180mJoint#3: 250-255 mJoint#4: 350-355mJoint#5: 440-445mJoint#6: 560-565mJoint#7: 670-675mJoint#8: 760-765mJoint#9: 890-895mJoint#10: 980-985mJoint#11: 1120-1125m
1.00E-05
1.50E-05
2.00E-05
2.50E-05
3.00E-05
3.50E-05
4.00E-05
0 20 40 60 80Current (A)
Volta
ge (V
olt)
1st test
After running thru 4" roller 3 times
After running thru 2" rollers 6 times
Wires with joints have to run through the reel-to-reel Ic test rig with 4” and 2”roller. No trace of degradation was shown in I-V curves
22EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Continuous multifilamentary 2G wire is now scaled to 15m lengths with new industrial process
4 mm
• Good Ic and reasonable ac loss reduction achieved;
• Coils were made with long length multifilamentary wires, showed lowered ac loss in magnetic field and with transport ac current as reported at DOE Peer Review (July 2008)
0.00 0.01 0.02 0.03 0.04 0.05 0.060
1
2
ac lo
ss (
W/m
)
Bac rms (T)
5.1 x
100 Hz unstriated
multifilamentary
23EPRI 8th Annual Superconductivity Workshop, November 12-13, 2008, Oak Ridge, TN
Customer-driven development of insulated wire
• Preliminary test showed no breakdown at 1000 V with 0.0025 mm polyimide film• Deliveries of insulated wire already being made.
• Several customers, primarily for coil applications, required insulated 2G wire• After evaluating a number of vendors, we procured a system for in-house
fabrication of insulated wire• System in place and being used for both 12 and 4 mm wide wire
1. AC Loss Characterization of HTS Coils
2. Proposed Integrated Cryo-cooled Test Bed for High Power Density Power System Components
Florida State UniversityCenter for Advanced Power Systems
Tallahassee
Sastry Pamidi
AC Losses With Liquid Nitrogen Boil-off Measurements
Useful for Total AC loss measurements on coils up to 140 mm in diameter and 250 mm tall.
Wide measurement range: fraction of a watt to 100 W
Coils can be arranged in any orientation with respect to magnetic field
Magnetic field amplitude: up to 200 mT
Transport current amplitude: up to 650 A
AC Losses in YBCO Coils with Nitrogen Boil-off Technique
Calibration Highly Reproducible
Sample Coil
Calibration Heater
Diameter - 145 mmLength - 250 mm
B
System has been tested and calibrated up to 60 W, 150 mT, 200 Hz
YBCO Coils, 29 turns, of wire ~4.5 m conductor 45 mm diameter, Ic = 32-34 A
Losses are < 0.1 W in parallel and perpendicular field 150 mT, 55 Hz & 60 mT, 200 Hz
AC Losses in YBCO Coils with Nitrogen Boil-off Technique
Super Power Coil Losses < 0.1 W
@ 150 mT, 55 Hz &60 mT, 200 Hz
Two coils were tested –Coil made of normal YBCO tape and Coil made of Striated YBCO ( five filaments). Both have < 0.1 W losses. 0.1 W is minimum detectable limit of the measurement system
Address system issues arising from the complex interrelationships between the electrical, thermal and material performance characteristic to achieve high power density systems through cryo-cooling.
Design and manufacture a 400 kVA, 13,8 kV HTS transformer for application in Test loop
Design and manufacture a +/- 5 kV MVDC HTS cable
Objectives of the Proposed Integrated Cryogenic System for Multiple High Density Power System Components
Flow sensors
Cryo booster
Temp sensors
Valves
Blowers
Electrical bushing
A Schematic of the Proposed Integrated Cryogenic System for Multiple High Density Power System Components
HTS AC/DC Cable
Main Cryostation HTS
Transformer
Capacitor Bank
HTS faultCurrent limiter
AC/DC
Converter
Load
Bank
Proposed Applications of Cryo-cooled Test Bed
Understanding of cryogenic system integration issues
For external users to test high density power devices
Comprehensive test environment with PHIL testing and heat loads and thermal gradients under test conditions
Demonstrate integrated high power density electrical network
1
Proposal of
9th Annual EPRI Superconductivity Conference
In Korea
2
Date From 9th Nov.(Monday) to 11th Nov.(Wednesday)
HostEPRI, KEPCO(KEPRI), and KIASC
* KIASC : Korea Institute of Applied Superconductivity and Cryogenics
Program
Committee
International Program Committee ;
• EPRI, KEPRI, KIASC
Local Program Committee ;
• KERPI, KIASC, KERI, LSC, KIMM, etc.
Conference
Site
KEPRI in Daejeon Korea (2 days)
Accommodation : Yusung Hotel, Rivera Hotel etc
Technical Tour : Gochang Test Field (1 day)
LS Cable Factory Tour (1day) : option
Outline Outline
3
Nov. 2008First Announcement(9th Annul EPRI Superconductivity Conference)
Feb. 2009 Website Opens
Aug. 2009 On-Line Submission of Abstracts
Sept. 2009 Abstract Acceptance & On-line Registration
Oct. 2009 Last Announcement with Final Program
Nov. 2009 Conference
Schedule (Tentative)Schedule (Tentative)
4
Conference Schedule (Tentative)Conference Schedule (Tentative)
First day ( KEPRI in Daejeon)
Registration
Presentation
Welcome Party and Dinner
Second day
Presentation
KEPRI Superconducting Lab Tour in KEPRI
Third day (Technical Tour : Gochang Test Field)
Move : Daejeon -> Gochang (by Bus)
Test Field Tour including 22.9kV and 154kV superconducting cable
Excursion : Sunwonsa Temple
4th Day (Option) : LS Cable Factory Tour
5
What benefit will you get ?
• You can contact with many experts from oversea
• You can get the current information on Superconductivity
System more broadly including Asia
• You can see the overall of the Superconductivity System. For
Example, HTS Cable, SFCL, Flywheel developed by Korea
• You can look around Gochang Test Center, specially new
underground test lab that is the biggest one in the world
through technical tour
• Lastly, you can enjoy beautiful sightseeing that may be great
mountain covered with colorful tree at Autumn
6
Technical TourTechnical Tour
Seoul
Busan
Daejeon
Gochang
7
Seoul
Busan
Daejeon
8
Testing Facility for HTS Cable by KEPCO
Place : Gochang Testing Center
Start : 2008.3
Finish : 2009.9
• 154kV Superconducting Cable Test will start 2009.6
9
KEPRI in Autumn KEPRI in Autumn –– Conference siteConference site
10
NaejangsanNaejangsan national Parknational Park
11
SunWonSaSunWonSa TempleTemple
High Opportunity Commercial Applications for HTS Cables
Eighth Annual EPRI Superconductivity ConferenceOak Ridge, TN ~ November 12 – 13, 2008
IntroductionIntroduction
• The scope and successful operation of recent HTS cable projects has led to:• Increased interest in HTS cables • Increased interest in their characteristics • Increased interest in possible applications
• Superconductor Cables are an Exciting New Tool for Utility Planning Departments, but requires:• Education on their benefits and applications• Education on what is involved to install and operate
• Agenda• Review of HTS cable applications which appear to be of
greatest interest during educational presentations • Issues moving forward
Key HTS Cable ELECTRICAL CharacteristicsKey HTS Cable ELECTRICAL Characteristics
• Very high power transfer capability compared to conventional cables solves many siting problems
• Very low impedance reduces loading on parallel lines and equipment
• Minimal magnetic field and elimination of heatsimplifies placement concerns and is easy on the environment
• Optional HTS cables with fault current managementcapabilities eliminate need to upgrade existing equipment
HTS Cables offer unique capabilities
Power Transfer Equivalency of HTS CablesPower Transfer Equivalency of HTS Cables
HTS Cables provide much greater power transfer than conventional cable
0 200 400 600 800 1000
13.8 kV
34.5KV
69kV
138kV
230kV345kV
Power Transfer Capability - 3Ø MVA
100 MVA at 13.8 kVXLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
HTS
HTS
HTS
HTS
* No XLPE cable de-rating factors applied. HTS rating based on conventional 4000A breaker rating
• Same Voltage, More Power• Greatly increased
power transfer capacity at any voltage level
• Same Voltage, More Power• Greatly increased
power transfer capacity at any voltage level
• Same Power, Lower Voltage• New MV versus HV
Siting Opportunity• “MV Transmission”• Ideal for NIMBY &
ROW sparse environments
HTS Cables provides transmission-level power transfer at medium voltage
0 200 400 600 800 1000
13.8 kV
34.5KV
69kV
138kV
230kV345kV
Power Transfer Capability - 3Ø MVA
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
HTS
HTS
HTS
HTS
* No XLPE cable de-rating factors applied. HTS rating based on conventional 4000A breaker rating
0 200 400 600 800 1000
13.8 kV
34.5KV
69kV
138kV
230kV345kV
Power Transfer Capability - 3Ø MVA
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
XLPE Cable
HTS
HTS
HTS
HTS
Power Transfer Equivalency of HTS CablesPower Transfer Equivalency of HTS Cables
Project HYDRA OverviewProject HYDRA Overview
Current ConEd System Configuration
ConEd’s System of the Future:• Interconnected Distribution Substations
• Integral Fault Current Limiting
Copper power cables HTS power cables
DHS Project supports development of a more resilient grid with increased reliability and reduced power outages
Paralleling Urban Buses Paralleling Urban Buses ––Building on Project HYDRA Building on Project HYDRA
• “Virtual Bus” must Handle high power flow between the substations• Conventional interconnection techniques not practical• Normal impedance during steady state operation would limit power transfer • Multiple cable circuits would be required
VIRTUAL BUSConnection
Paralleling low-side buses with conventional technologyis not practical
Typical 2-transformer urban substations
Paralleling Urban Buses: HTS SolutionParalleling Urban Buses: HTS Solution
HTS Cable Advantages• Low impedance allows for efficient power transfer• Ampacity of HTS cable capacity requires only one circuit
• e.g. 100MVA at 15kV• Reduced external EMF and heat generation simplifies placement
4000A
HTS Cable Enables Low Side Interconnection
Load Current
Typical 2-transformer urban substations
Paralleling Urban Buses:Paralleling Urban Buses:Addressing Fault CurrentsAddressing Fault Currents
Fault Current Limiting HTS Cable provides many benefits:• Reduces the fault current that flows through the HTS cable• Reduces fault current contribution to faults on either substation bus• Eliminates need to replace or upgrade station equipment
60,000A
Fault Current Limiting HTS Cable makes low side networking practical
Fault CurrentContribution
30,000AReduced Fault CurrentContribution
With Fault Current Limiting HTS Cable
Typical 2-transformer urban substations
Paralleling Urban Buses: Paralleling Urban Buses: The AppealThe Appeal
Advantages of Paralleled Substations – Simple Case• Connect additional load without additional transformers or new substations• Increases transformer asset utilization• Reduces cost of N-1 contingency planning; Only 1 transformer required
versus 2• Increased interconnectivity protects vulnerable, critical loads in the event of
a catastrophic failure
Typical 2-transformer urban substations
Paralleling Dense Urban Load Centers Leads to Operational Efficiencies
Total Load ≤60% total transformer MVA Total Load ≤60% total transformer MVATypicalLoadingPractice
Paralleling Urban BusesParalleling Urban BusesIncreased Asset UtilizationIncreased Asset Utilization
Transformer Asset Utilization TS Inteconnected Substations; n-2 Criteria
30%
40%
50%
60%
70%
80%
90%
100%
None 2 3 4 5Number of Interconnected Substations
Tran
sfor
mer
Ass
et
Util
izat
ion
3 XFRMR4 XFRMR5 XFRMR
Interconnecting Substations increases transformer asset utilization*• Improves financial performance measures• Reduces the number of transformers required to serve load
* Theoretical limits
Transformer Asset Utilization TS Inteconnected Substations; n-1 Criteria
30%
40%
50%
60%
70%
80%
90%
100%
None 2 3 4 5Number of Interconnected Substations
Tran
sfor
mer
Ass
et
Util
izat
ion
2 XFRMR3 XFRMR4 XFRMR5 XFRMR
Paralleling Urban BusesParalleling Urban BusesServing Additional LoadServing Additional Load
HTS Interconnected Substation Loading Increase Capability; n-2 Criteria
0%
20%
40%
60%
80%
100%
120%
140%
160%
180%
2 3 4 5Number of Interconnected Substations
% In
crea
sed
Load
C
apab
ility
3 XFRMR4 XFRMR5 XFRMR
Interconnecting Substations significantly increases load serving capability*• Significantly reduces need to expand or build new substations
* Theoretical limits
HTS Interconnected Substation Loading Increase Capability; n-1 Criteria
0%10%20%30%40%50%60%70%80%90%
100%
2 3 4 5Number of Interconnected Substations
% In
crea
sed
Load
C
apab
ility
2 XFRMR3 XFRMR4 XFRMR5 XFRMR
Segregated (Remote) SubstationSegregated (Remote) Substation
• Smaller, remotely located, lower voltage switching station in space or real-estate constrained location
HTS CABLE
• Larger, HV station components located where space is available
• MV HTS cable acts as low impedance, high capacity, virtual bus between transformer and switching stations
• Reuse existing ROW• Simplified placement due to lower
voltage level• FCL HTS cable may reduce MV
breaker requirements
Permits new substation construction in spite of severe real estate constraints
Segregated (Remote) SubstationSegregated (Remote) Substation
HTS CABLE
HTS Cables can be consistent with tradition reliability design practices
HTS CABLE
• Multiple HV stations located where space is available to provide for contingency planning
• MV HTS cables provide links and fault current control
Overcoming Transmission Line Overcoming Transmission Line Siting DilemmasSiting Dilemmas
HTS Cables Very Attractive to Address Transmission Siting Issues
• Underground construction• Preferred by the public• Better storm performance• HTS offers simplified
burial requirements• Space efficient
• Lower voltage option simplifies siting
• Environmental benefits• No EMF emissions • Environmentally friendly
insulation system• Positive public relations
Power system reliability and load growth requires new interconnections to strengthen the grid and supply new load
GG
GG
Substation A Substation B
Simplifying Transmission SitingSimplifying Transmission Siting
HTS Cables Offer New Options to Siting Power LinesPhoto courtesy Consolidated Edison
One MV HTS Cable can replace:• Many conventional underground
circuits• Overhead transmission line
One MV HTS Cable can replace:• Many conventional underground
circuits• Overhead transmission line
Connecting Generating Stations to GridConnecting Generating Stations to Gridor Any Short, High Power Linkor Any Short, High Power Link
HTS Section for sensitiveor ROW restricted areas
G
G
G
G
HTS Cables Can Ease or Eliminate or Simplify Short Link Issues
GenerationStation
Grid PCC
• Advantageous for short, high power transfer situations• Permits use of more compact, easier to site, lower voltages• Environmentally and politically preferable underground
construction• Lower losses
• Ideal for routes including sensitive or ROW restricted areas
Conventional constructionfor balance of link
Grid CongestionGrid Congestion
Line loading, equipment & operational limitations can lead to grid congestion
Grid Congestion has many causes• Insufficient line ampacity• Overloaded critical assets and
circuits• Undesired loop flows• Stability issues
GG
UndesiredLoopFlow
GGGenerationGeneration
LoadLoad
Load Current
Load Current
HTS Cable Can Alleviate Grid CongestionHTS Cable Can Alleviate Grid Congestion
• During normal operating conditions, the HTS cable is a low impedance pathand allows for the transfer of large amounts of power.
HTS CableHigh Normal Current
Low Fault Current
Numerous benefits accrue:• Increased corridor transfer capability of the corridor• Reduced loading on parallel circuits• Improved efficiency from lower I2R losses on all lines
GG
Load Current
GGGeneration
Load
Load Current
Load Current
Reduced line
losses
Increased line
loading
Reduced loading
on assets
During Faults HTS Cable Limits Fault CurrentsDuring Faults HTS Cable Limits Fault Currents
• When an HTS cable with resistive FCL capability becomes resistive during a fault, the fault current must use relatively lower impedance paths
HTS CableHigh Normal Current
Low Fault Current
The HTS cable results in higher system impedance during faulted conditions lowering overall fault current magnitudes
GGFaultFault
Fault Current
FaultCurrent
GGGenerationGeneration
Increased Fault impedance increases
total circuit fault impedance
Conventional Vs. Project Hydra Style HTS CableConventional Vs. Project Hydra Style HTS Cable
ScenarioMVA Transfer
Capacity Increase Sub#1 Sub #2
Base Case 230 MVA Base 42 kA 56 kA
2nd Conventional Cable +230 + 5 +2
Replacement HTS Cable +248 -12 -3
Fault Current Level Change (kA)
Installing HTS Cable in the grid simultaneously can increase power transfer capability and manages fault current levels
SummarySummary
• HTS Cable Systems offer solutionsunavailable or impractical until now
• As utilities are exposed to HTS cableconcepts, applications become apparent
• Most utility personnel have had little exposure to HTS cables andtheir characteristics
• This exposure is for the most part limited to a utility’s advanced technology or R&D functions• i.e., those that are exposed to normal planning issues are not
considering HTS solutions• The industry must undertake an Educational Awareness program to
ensure HTS cables become part of the engineer’s toolset
•HTS cable applications are nascent•Education is required to spur demand
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Development of HTS Cables for DC Power Transmission and Distribution
Joseph V. MinerviniLeslie Bromberg
Makoto TakayasuChristopher Miles and Nicholas R. LaBounty
MIT Plasma Science and Fusion Center
Eighth Annual EPRI Superconductivity ConferenceDoubletree, Oak Ridge, TN ~ November 12 – 13, 2008
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering DivisionOutline
• HTS DC Advantages• Cable Design Concepts• Chubu-MIT HTS DC Cable Collaboration• Long Length Cooling• Current Lead Cooling• Potential Near Term Application• Conclusions
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering DivisionDC Superconducting Transmission Line
Advantages:•No DC resistive losses•No AC inductive storage•Low or no AC losses•Long range transmission of high currents, including undersea•Very high power ratings including transmission of several GVA •Fault currents limited by fast acting inverters at AC/DC and DC/AC ends of the line•Low voltage transmission, if desired, limiting the need for high voltage transformers•Simplified cable design, more amenable to using HTS tape geometry•Cable coolant also used to cool solid state inverters increasing capacity and reducing high temperature aging degradation
Disadvantages: Invertors can add substantially to cost
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
HTS DC increases efficiency for long distance transmission Opens other advanced technology opportunities:
• Direct connection of alternative low-carbon or carbon-free power sources:WindSolar PVFuel CellMicroturbineother
• Connection of advanced energy storage devicesFlywheelBatterySupercapacitorSuperconducting Magnetic Energy Storage (SMES)other
HTS DC Applications
Grid independence
System Stability and Power Quality
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
HTS DC Transmission Cables
DC-to-AC Power Conversion
Off-Shore Wind Farm Power Transmission
Using HTS DC Cable
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Solar Photovolatic or Concentrated Solar Thermal Power Transmission Using HTS DC Cable
Solar PV CSP
Solar and WindDC Power
Transmit DC before conversion?
DC Superconducting Power Transmission Line Experiment in
Chubu University&
Collaboration with MIT
Prof. Satarou YamaguchiDept. of Electrical Engineering
Center of Applied Superconductivity and Sustainable Energy Research
(CASER)
Experimental Device in Chubu University
Parameterscurrent > 2.5 kAvoltage > 20 kVlength ~ 20 mSumitomo Bi-2223 cable
coolant; LN2equipped with pump and cryogenic cooler72 K - 77 K
SC Cable
made by Sumitomo
insulation layer
HTS Tape
formercopper wires
inner spring
center holefor coolant path
Photo of cross-section
40φ
insulation30kVDC
earth layer
formercopper wires
HTS Tape x 39
Side View
Tape conductor 1st layer; 192nd layer; 20
Bi-2223/ 100A grade
Insulation Volt. DC20kV Insulator, PPPL
Outer radius 40φ Center hole 14φ
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering DivisionMIT High Current HTS
DC Cable Designs
Multiple Layers
Triplet
Carpet Stack
Twisted Triplets
Wedge Stack
Twisted Triplets
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
• Use Basic Carpet Stack– tapes can be insulated or soldered• Square or rectangular stack • Base element former can be– conducting– non-conducting– Structural• Tape shape requires relatively long twist
pitches• AC losses not an issue for DC applications
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
• 25 kA at T = 65 K - 77 K• Carpet Stack triplets have highest Je• Allows for smaller cryostat and lower heat leak• Carpet Stack and wedge base conductors allow many
variations on cable patterns and total tape number
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division Potential OpportunityData Server Centers
• In 2006, electricity consumed by servers in U.S. data centers (including cooling and auxiliary infrastructure) represented about 1.5 percent of national electricity use*.
• Internet data center consumes ~ 1–2 kW/m2.– 10 MW-50 MW+ total capacity in new centers
• DC may be preferred– Minimizes conversion losses
• ~7-10% energy savings migrating to DC– No reactive power– Power multiplier: for 1 W dissipation saved, 1.5 - 2 W
cooling eliminated
Google datacenter near The Dalles Dam
*”Report to Congress on Server and Data Center Energy Efficiency”, U.S. Environmental Protection
Agency, Aug. 2, 2007
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Expected Data Server CenterPower Growth
G. Lawton, Powering Down the Computing Infrastructure, Computer, IEEE, 40, issue 2, p 16-19, Feb. 2007.
DC Distribution Demonstration Developed by LBNL and Industry Partners
William Tschudi, LBNL
Measured Best in Class AC System Loss Compared to DC• ~9-12% efficiency improvement measured by elimination of transformer
and second AC/DC conversion
PSU
ASD
Ballast
AC Distribution
Electronicloads
Lightingloads
Motorloads
AC/DC
AC/DC
VRAC/DCDC/DCAC/DC DC/AC
DC/AC
DC/AC
60 Hz AC480V
AC/DC DC/AC
DC/ACDC
300-400V
PV
FC
Benefits of 400Vdc
Slides courtesy of Annabelle Pratt-Intel
PSU
ASD
Ballast
Facility Level
Electronicloads
Lightingloads
Motorloads
AC/DC
AC/DC
VRAC/DCDC/DCAC/DC DC/AC
DC/AC
DC/AC
60 Hz AC480V
AC/DC DC/AC
DC/ACDC
300-400V
PV
FC
Benefits of 400Vdc
Slides courtesy of Annabelle Pratt-Intel
XX
XXXX
XXXX XX
XX
XX
ASD
PSU
Ballast
400V DC facility with DG
60 Hz AC480V
Electronicloads
Lightingloads
Motorloads
VRDC/DC
AC/DC
DC300-400V
DC/AC
DC/AC
Benefits of 400Vdc
AC/DC
DC/DC
DC/DC
Slides courtesy of Annabelle Pratt-Intel
ASD
PSU
Ballast
400V DC facility with SC Bus
60 Hz AC480V
Electronicloads
Lightingloads
Motorloads
VRDC/DC
AC/DC
DC300-400V
DC/AC
DC/AC
Benefits of 400Vdc
AC/DC
DC/DC
DC/DC
Slides courtesy of Annabelle Pratt-Intel
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division 4400 Ampere Cable Sizes
1.75” Diameter cable325 A per cable
14 Cables35 lbs/ft
0.605” Diameter cable133 A per cable
33 Cables8 lbs/ft
1.75” Diameterup to 30 Conductors
up to 200 Amps per Conductor1 Cable2.0 lbs/ft
Copper - Air cooled Copper - Water cooled HTS- LN2 Cooled
Very High Power Density is Achievable with Superconductors
x 10 = 4000 A @ 0 Voltage ®
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Schematic 10MW, 400V, 25 kAData Center Layout
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Technology Needed to ImplementSC Distribution
• As opposed to transmission, there are a large number of secondary spurs, with relatively high density (depending on application)
• Refrigeration losses dominated by leads, not by distributed cryostat or AC losses
• Need to address the problem of– Electrical connections through low-loss leads– Cooling manifolding
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Navigant Consulting costing predictions of SC components in 2008-2012:http://www.energetics.com/meetings/supercon06/pdfs/Plenary/07_Navigant_HTS_Market_Readiness_Study.pdf
Power Dissipation with Standard Leads (kW)
Summary of Preliminary System AnalysisMIT Energy Initiative Seed Fund - 2008
Current lead loss is 0.05 W/A-lead
Power Loss HTS + Cu
(2007)
Power Loss HTS + Cu (2008-2011)
Power Loss HTS + Cu (2012-2016)
Power Loss All Cu
HTS Leads 10 10 10
HTS Cryostat 0.45 0.225 0.225
HTS Cold Power Total 10.450 10.225 10.225
Refrigerator Wall Power 300 177 118
Copper Bus 16 16 16 250
Total Electrical System Power 316 193 134 250
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Navigant Consulting costing predictions of SC components in 2008-2012:http://www.energetics.com/meetings/supercon06/pdfs/Plenary/07_Navigant_HTS_Market_Readiness_Study.pdf
Power Dissipation with Optimized Leads (kW)
MITEI Seed Fund Study (cont’d)
Current lead loss is 0.025 W/A-lead achieved by intermediate cooling stage
Power Loss HTS + Cu
(2007)
Power Loss HTS + Cu (2008-2011)
Power Loss HTS + Cu (2012-2016)
Power Loss All Cu System
HTS Leads 5 5 5
HTS Cryostat 0.450 0.225 0.225
HTS Cold Power Total 5.450 5.225 5.225
Refrigerator Wall Power 157 90 60
Copper Bus 16 16 16 250
Total Electrical System Power 173 106 76 250
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Navigant Consulting costing predictions of SC components in 2008-2012: http://www.energetics.com/meetings/supercon06/pdfs/Plenary/07_Navigant_HTS_Market_Readiness_Study.pdf
Capital Costs (k$)
MITEI Seed Fund Study (cont’d)
Capital Costs HTS + Cu
2007
Capital Costs HTS + Cu 2008-2011
Capital Costs HTS + Cu 2012-2016
Capital Costs All Cu
HTS Tape 2,800 560 112
HTS Cryostat 200 130 44
HTS Refrigerator
1,050 640 260
HTS Total 4,050 1,330 416
Copper Bus 11 11 11 160
Total Capital Cost
4,061 1,341 427 160
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division
Operating Costs of Power ($/Hr)
Electricity cost = $0.10/kW-Hr
MITEI Seed Fund Study (cont’d)
Operating Costs 2007
Operating Costs
2008-2011
Operating Costs
2012-2016
HTS (standard leads) 31.69 19.27 13.38
HTS (optimized leads) 17.26 10.62 7.61
All Copper 25.07 25.07 25.07
HTS Payback Period (standard leads)
Never 23 Years 2.6 Years
HTS Payback Period (optimized leads)
57 Years 9.2 Years 1.75 Years
Portions reprinted, with permission, from Massachusetts Institute of Technology and Joseph Minervini.
Technology & Engineering Division Summary
Use of HTS could open innovative opportunities in datacenters for decreased power consumption, flexibility and easy of constructionApplication to data server centers is a near term application with potential large efficiency gainsShort time scale implementation allows further development for other MicroGrid applications with similar technologyEstablishes technology for:
• Bringing large-scale power to land from offshore wind farms
• Combining large-scale solar PV or solar thermal systems to the grid
• Long distance power transmission and/or grid interconnects
Optimized DC cable, cryostat and current leads require development program
A High-Power Superconducting DC Cable
W. V. Hassenzahl
Eighth Annual EPRI Superconductivity Conference
11/13/2008
Outline
• The team• Visions Past and Present• Why a superconducting DC cable• Program goals• Design concept• Design process
11/13/08 2An SC-DC Cable
The team
• Steve Eckroad• Bill Hassenzahl• Paul Grant• Brian Gregory• Stig Nilsson
11/13/08 3An SC-DC Cable
Why a SC DC Cable
• High Power Capacity pluses and minuses• Negligible losses resistive and AC • Physical Dimensions Small vs. Power Lines• Security • High Current and Relatively Low Voltage• Reliability• Versatility• Efficiency Lower Life Cycle Cost
11/13/08 4An SC-DC Cable
Why operate near 77 K?• To answer this question we need to explore conductor costs and the
life cycle energy demands of an installed cable
11/13/08 5An SC-DC Cable
Why operate near 77 K?• To answer this question we need to explore conductor costs and the
life cycle energy demands of an installed cable
11/13/08 6An SC-DC Cable
CautionComparisons aremodel specific.
Why A DC Cable near 77K?• 77 K a real sweet spot
11/13/08 7An SC-DC Cable
Program Goals• Design a Superconducting DC Cable System that
meets future utility needs and requirements.– Recognize high power limitations of local AC system– Assess power levels and cable lengths– Note power independent costs of proposed design
• Use existing engineering capability for materials and fabrication processes.
– Structural Materials– Cryogenics and vacuum– Power Converters– Superconductors
• Not the driver!
11/13/08 8An SC-DC Cable
2 SC DC Cable Systems• Assessed power levels and cable lengths
– Selected two cable systems for Reference Designs• Regional 2 GW <300 km• Inter regional 10 GW >500 km
– Established a simple set of design requirements • multiple power feeds and loads• redundant cables in each circuit• redundant converters
• Iterative Process– Power Levels, Ranges, and Limits I and V– Conductors, other materials, standard practices
Metal Sheath OD and Vacuum shell piece length – Metal Sheath OD and Spool Sizes
Cable section lengths, i.e., Unit length between joints– Heat loads Cryogenic Requirements
Fluid Flow Area Cryogenic Diameter and stop joint– Vacuum requirement Outer Shell ID
11/13/08 9An SC-DC Cable
Power Ranges - I and V
• Regional 2 GW1 GW per SCDC CableEach cable has full capacity for redundancy ~33.3 kA and ~60 kV*
• Inter Regional– up to 10 GWE.g., power farm to major loads
5 GW per HVDC CableEach cable has full capacity for redundancy ~100 kA and ~100 kV
* May choose 100 kV
11/13/08 10An SC-DC Cable
Design Concept • Details of cross section
depend on operational conditions
• Figure includes recent changes to accommodate ground issues raised by AC/DC Integration team
• Approximate diameter 12 cm
11/13/08 11An SC-DC Cable
Cable Section Length
• V, I, and material properties determine – Metal Sheath OD– Cable weight per meter of length– Note mechanical properties of insulation require a
larger minimum thickness than does voltage standoff• Metal Sheath OD, spool dimensions, and required
pulling force determine– cable section length from spreadsheet
• Manhole or other access capability required at end of each section for joint preparation
• Experience with conventional cables is applicable
11/13/08 12An SC-DC Cable
Heat Loads
• Heat sources– Conduction– Convection– Radiation– AC losses = hysteresis from current changes and ripple– Cable ends / joints– Cryogen flow losses
• Use nominal heat load of 1 W/m for initial calculations.
11/13/08 13An SC-DC Cable
AC Losses• Two types of heat input in the superconductor
– Current ramping and faults– Harmonic currents
• Several methods for calculating heat input.– Abrupt current decrease can only deliver energy
associated with inductance per unit length L/l• Energy goes into enthalpy of nitrogen ΔT<0.01K
– Harmonic currents set limits on converter design and operation
∑ ⋅⋅≅ −
n_all
2nn
7 I104)m/W(P ω
11/13/08 14An SC-DC Cable
Vacuum • Conduction and convection heat load must be < 0.5 W/m
depends on use of mli and quality of vacuum• Required vacuum about 2x10-4 Torr
– First approach permanently sealed system with getters• Not feasible to guarantee >500 km without leaks.
– Second approach vacuum pumps at fixed spacing• Issue is pressure increase from pump to furthest point requires
large open cross section• Calculation of spacing is based on gas flow from largest leak,
conductance of the cable vacuum space, and vacuum pump capacity.• Determine that a 0.7 m pipe, 50 liter/s, 10-4 Torr vacuum pumps
with every km will meet vacuum needs even if some pumps fail.• Pumps need not work full time after operation begins• Also, pumps must be able to pump down the cable prior to use
Pump spacing is intimately connected with maximum cable piece length11/13/08 15An SC-DC Cable
Cryogenics• Superconductivity requires a low temperature
– 65 to 70 K for liquid nitrogen– Over distances of a 1000 km– Small temperature variations
• Normal operation ± ~ 1 K• Upset/fault conditions > +5 K
• Requires pressurized flow of liquid nitrogen– Pressure of several atm required to limit bubble formation
and to maintain consistent dielectric strength– This “low” pressure allows the use of thin walled pipes– Which, in turn, limits the allowable pressure rise caused by
flow resistance
11/13/08 16An SC-DC Cable
Cryogenics• Refrigerator loads and separation
– Choice of capacity of each refrigerator depends on• Total heat inflow between refrigerators• Need for on line maintenance• Operation during and after upset/fault conditions• Cool down• Cost vs. capacity factors (Optimization for the future)• Iterative process among heat load, refrigerator spacing, reliability, etc.
– A pressure rise of 2.5 atm. is allowable for an operating pressure of 5 to 10 atm.
– A flow rate of 5 liters/s can remove 10 kW– The associated pressure rise in 10 km is ~3 atm, 45 psi.– Choose 5 to 10 km refrigeration spacing.
11/13/08 17An SC-DC Cable
The grid should not know about refrigerators
Pumping/friction power is about 0.2 W/m
Cryogenics Summary
• Heat load, allowable temperature rise determine– Minimum cryogen mass flow
• Cryogen mass flow and allowable pressure drop determine
– total refrigerator capacity and refrigerator spacing.• Refrigerator spacing is an optimization issue.
– 5 to 10 km is adequate with a 3 to 5 atmosphere pressure drop for liquid nitrogen.
Part of iterative design, but not a driver
11/13/08 18An SC-DC Cable
Design Concept
11/13/08 19An SC-DC Cable
Factory Assembly
• Outer pipe– Standard high pressure gas pipe– Special welding and cleaning– Reflecting surface on inner diameter– Environmental protective outer coating – Piece length determined by shipping constraints (?~20 m)
• Cryogenic pipe and cryogen return pipe– Corrugated stainless steel– Special weld requirements– Supported at each end from outer pipe
• Superinsulation– Most important 30 to 50 layers between outer pipe and
cryogenic components– A few layers between the two cold pipes.
11/13/08 20An SC-DC Cable
Pipe Section and Transport
11/13/08 21An SC-DC Cable
On Site Assembly
11/13/08 22An SC-DC Cable
This procedure is followed for some 50 sections
Vault and Cable Pulling
11/13/08 23An SC-DC Cable
Joints
11/13/08 24An SC-DC Cable
Joints• Cable joint Issues
– Large number of superconductor tapes/wires– Field procedures especially repairs– End connections and terminations
• Pipe joint characteristics determined by – Manufacturability– Cleanliness– Superinsulation protection– Accommodation of cable pulling loads– Thermal contraction associated with cooldown
11/13/08 25An SC-DC Cable
Cable Installed
11/13/08 26An SC-DC Cable
Cryogenic Vault
11/13/08 27An SC-DC Cable
Outer Pipe Summary• Outer pipe diameter >70 cm determined by
– Cryogen pipe diameter– Vacuum pressure drop– Vacuum pumping requirements with redundancy
• Outer pipe piece length determined by transportability ~ 20 m maybe 30 m max
– Fabricate in plant with mli and cryogen tube • Includes supports for axial and radial motion of cold
components• Seal in factory for cleanliness
• Assemble (weld) pipes and cryogen tubes on site and pull cable from ends.
11/13/08 28An SC-DC Cable
Gas Pipeline
11/13/08 29An SC-DC Cable
SC-DC Cable Program Status
• Critical issues for future evaluation– Cable piece length – Power converter and grid interface– Other existing and new superconductors– 100 kA joints– Temperature optimization– Allowable heat loads– Vacuum requirements– Details of refrigerator mechanical interface to cable– Overall cost evaluation
11/13/08 30An SC-DC Cable
1
Power Flow and Transient Stability Impacts of
Superconducting DC CablesTom Overbye
University of Illinois and PowerWorld Corporation
Eighth EPRI Superconductivity ConferenceNovember 12-13, 2008
This presentation is based on work is being performed under contract with EPRI
Overview
• Goal of this work is to consider the power flow and transient stability impacts of integrating a multi-tap, superconducting DC (SCDC) cable system within the Eastern Interconnect and within the WECC system.– Power levels are up to 10 GW
• A dual SCDC cable system is assumed, with the ability to failover with full power in the event of a fault on one of the cables. – Analysis compared different failover scenarios with
remaining cable ramping to full power over a few seconds– After failover full power is assumed on the remaining cable
Eastern Interconnect Study System
• The system studied was the NERC/MMWG 2008 summer peak case from the 2006 series.
• Case has 48,370 buses, 7397 generators, a total load of 660 GW and total generation of 676 GW.
• 2006 series dynamic models.• Power flow and transient stability runs were done
using PowerWorld Simulator version 14.• As is common with the MMWG cases, there were
many initial line violations (330 lines at >= 100% of A limit MVA, 95 lines >= 120% of A limit MVA)
Eastern Interconnect Route for 10 GW Cable System with Six Stations
2000 MW
2500 MW
2000 MW
1500 MW
2000 MW
10,000 MW of Asynchronous Generation
System Modifications
• System was modified to include the SCDC cable system by adding five new buses (100001 to 100005) with their generation set to match SCDC cable injections. Buses were then connected to existing buses by short lines:– Bus 100001 to 36260 (2.5 GW) Chicago South– Bus 100002 to 36421 (2.0 GW) Chicago North– Bus 100003 to 31230 (2.0 GW) St. Louis– Bus 100004 to 57968 (1.5 GW) Kansas City– Bus 100005 to 54901 (2.0 GW) Oklahoma City
• The remote source generator(s) was assumed to be operating asynchronous with the rest of the grid.
System Modifications, cont.
• Existing generation in areas with SCDC cable injections was reduced to satisfy area ACE requirements.
• Once the SCDC cable injections were modeled, two new 345 kV lines needed to be added to reduce line loadings.– Between buses 57977 57968 (South of Kansas City)– Between buses 57968 59200 (South of Kansas City)
• System with SCDC cable was not augmented to make it n-1 secure, but there were no significant base case violations.
Example: Original Kansas City Area Flows and Voltages
Kansas City Area Flows and Voltages with SCDC Cable
Power Flow Conclusions
• Integration of the SCDC cable within the existing system will require modifications to the transmission grid similar to those needed to accommodate a new power plant of similar size or a new high voltage transmission line with similar capacity.
• Any new voltage problems can be corrected by new reactive control devices, such as capacitors or SVCs.
• Flow changes caused by cable failure would be rapidly corrected by power transfer to the unfaulted cable.
• Conclusion: From a power flow perspective the integration of the SCDC system is straightforward.
Transient Stability Analysis
• Transient stability analysis, the study of whether all the system generators will retain synchronism following a system disturbance, is a critical question.
• The assumed fault scenario was to apply a balanced, three phase, solid fault at each of the five SCDC cable terminals. The fault was then cleared after three cycles (0.05 seconds). Different scenarios were then considered for the pick in the SCDC injections:– None (both cables failed)– Half (no transfer of power from the faulted cable)– Half, then ramp to full over either 1 second or 5 seconds
Frequencies for All Generators; Complete Loss of Both Cables
Values are generator frequencies in HzMinimum Frequency is about 59.58 Hz
Frequencies for Selected Generators; Complete Loss of Both Cables
Example of Governor Response for Loss of 10 GW
Gen 1GASTON5 #5 Mech Input
Gen 1GASTON5 #5 Mech Input
Time in Seconds1514131211109876543210
Gen
1G
ASTO
N5
#5 M
ech
Inpu
t
860
859
858
857
856
855
854
853
852
851
850
849
848
847
846
845
844
Given a loss of 10 GW for a 676 GW system,a proportionalgeneration increasefor this generatorwould be 0.844/676*10 GW= 12.4 MW. Actual is slightly different becauseof differing gover-nor characteristics
Frequencies for All Generators; Loss of One Cable; No MW Transfer
Minimum Frequency is about 59.70 Hz
Frequencies for Selected Generators; Loss of One Cable; No MW Transfer
Frequencies for All Generators; Loss of One Cable; 5 Sec MW Ramp
Minimum Frequency is about 59.70 Hz
Frequencies for Selected Generators; Loss of One Cable; 5 Sec MW Ramp
Example of Governor Response for 5 Second Ramp Recovery
Gen 1GASTON5 #5 Mech Input
Gen 1GASTON5 #5 Mech Input
Time in Seconds1514131211109876543210
Gen
1G
ASTO
N5
#5 M
ech
Inpu
t
849
848
847
846
845
844
In previous plot forthis governor (for thecomplete loss ofboth cables case)the output went up to860 MW. Now inrecovers quite quickly to its pre-contingency value
Frequencies for All Generators; Loss of One Cable; 1 Sec MW Ramp
Minimum Frequency is about 59.72 Hz
Frequencies for Selected Generators; Loss of One Cable; 1 Sec MW Ramp
Frequency Response Discussion
• With no (or slow) power recovery the maximum frequency drop was about 0.3 Hz (done to 59.7) when only one cable failed (5 GW loss)– Well above highest load shed frequency of 59.3 Hz.
• Likely drop could be more because– Study considered peak summer load condition, which has
more generators spinning– Transient stability cases tend to under-estimate frequency
decline since not all governors are available
• But the modeled frequency decline tends to match actual results (see next slide)
April 23, 2002 Frequency Response Following Loss of 2600 MW
Decline for 2600MW was about 0.1 Hz, so 0.3 Hzfor 5000 MW is actually slightlyhigh. But chart atleft 1) only showsthe frequency at one location, notthe lowest frequencyand 2) measurementdelay may havemissed the lowestvalue.
Historical Eastern Interconnect Frequency Response
23
Source: “Interconnected Power System Response to Generation Governing: Present Practice andOutstanding Concerns,” IEEE Task Force on Large Interconnected Power System Response,IEEE Publication 07TP180, May 2007 (Figure 2-22)
Our valueswere about1700 MW/0.1Hz for the 5 GW loss case(one cable)and 2500 for the 10 GWLoss case(both cables)
Frequency Propagation Animation
• The accompanying slide set shows an animation of the frequency for the first four seconds for the 5 second ramp recovery case.
Eastern Interconnect Transient Stability Conclusions
• From a transient stability point of view, a 10 GW SCDC cable could be integrated into the existing Eastern Interconnect.
• Frequency response is fairly insensitive to how quickly the power is transferred from faulted cable to the unfaulted cable (one versus five seconds)– Transfer time does affect how much power needs to be picked
up by the generator governors, and for how long.
WECC System
• The system studied was the WECC 2010 LA1-SA Approved Base Case.
• Case has 15,795 buses, 3100 generators, a total load of 106 GW and total generation of 111 GW.
• 2006 series dynamic models.• Power flow and transient stability runs were done
using PowerWorld Simulator version 14.• Case had several minor initial flow violations.
Power flow and contingency limits were not considered
26
WECC SCDC Cable Route: Six Stations, 8.5 GW
27
8500 MW Asynchronous Generation
Denver: 1500.0 MW
Alburquerque: 1000.0 MW
Phoenix2000.0 MW
SanDiego: 1500.0 MW
Los Angles: 2500.0 MW
Freq. Deviation for All Generators; Loss of One Cable: Worst Case
28
Freq. Deviation for All Generators; Loss of One Cable; 8 Sec MW Ramp
29
Freq. Deviation for All Generators; Loss of One Cable; 4 Sec MW Ramp
30
Freq. Deviation for All Generators; Loss of One Cable; 2 Sec MW Ramp
31
Freq. Deviation for All Generators; Loss of One Cable; 1 Sec MW Ramp
32
Comparison with ActualWECC Frequency Results
33
Source: L. Pereira, et. al., “New Thermal Governor Model Selection and Validation in the WECC,” IEEE Transactions on Power Systems, February 2004, pp. 517-523 (Figure 1).
WECC FrequencyResponses Tendsto be Around800 or 900 MW/0.1 Hz. So a 4.25 GWsustained loss would result in an anticipated frequency declineof close about 0.5 Hz, slightly above the 59.3 load shed threshold.
WECC Transient Stability Conclusions
• From a transient stability point of view, an 8.5 GW SCDC cable could be integrated into the existing WECC Interconnect provided following a fault the power can be quickly transferred to the unfaulted cable.
• Quick power transfer (several seconds maximum) can reduce the point of maximum frequency dip, which occurs at about five seconds in both the simulations and with actual system results.
34
1
Slides Show Locational Variation in Bus Frequency for the 5 Second Ramp Eastern Case
This presentation is based on work is being performed under contract with EPRI
Tom OverbyeUniversity of Illinois and PowerWorld Corporation
Eighth EPRI Superconductivity ConferenceNovember 12-13, 2008
Transient Stability Frequency Animation: Time = 0.0 Seconds
Time: 0.1 Seconds
Time: 0.2 Seconds
Time: 0.3 Seconds
Time: 0.4 Seconds
Time: 0.5 Seconds
Time: 0.6 Seconds
Time: 0.7 Seconds
Time: 0.8 Seconds
Time: 0.9 Seconds
Time: 1.0 Seconds
Time: 1.1 Seconds
Time: 1.2 Seconds
Time: 1.3 Seconds
Time: 1.4 Seconds
Time: 1.5 Seconds
Time: 1.6 Seconds
Time: 1.7 Seconds
Time: 1.8 Seconds
Time: 1.9 Seconds
Time: 2.0 Seconds
Time: 2.1 Seconds
Time: 2.2 Seconds
Time: 2.3 Seconds
Time: 2.4 Seconds
Time: 2.5 Seconds
Time: 2.6 Seconds
Time: 2.7 Seconds
Time: 2.8 Seconds
Time: 2.9 Seconds
Time: 3.0 Seconds
Time: 3.1 Seconds
Time: 3.2 Seconds
Time: 3.3 Seconds
Time: 3.4 Seconds
Time: 3.5 Seconds
Time: 3.6 Seconds
Time: 3.7 Seconds
Time: 3.8 Seconds
Time: 3.9 Seconds
Time: 4.0 Seconds
November 12 & 13, 2008
Eighth EPRI Superconductivity Conference
Issues Associated with a Superconducting DC Line
Fed by a Multi‐Terminal VSC System
Tom Baldwin, Florida State Univ.Paulo Ribeiro, Calvin College, and Brian Johnson, Univ. of Idaho
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 2
Outline
• Enabling Technologies:– High Power Voltage Source Converters– DC Superconducting Cables
• Topologies– Multi‐Tap VSCs Issues
• DC Power Control– Rectifiers / Inverters– Dealing with Transient Current/Power Variations– Practical Power and Current Limitations
• Discussions
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 3
SCDC Control Analysis and Simulations
• Cable model from– W. Hassenzahl, “A high‐power superconducting dc cable, an EPRI program”
SCDC Project Review Meeting, Charlotte, NC, 10 December 2007
• System model from– S. Nilsson and A. Daneshpooy, “Simulation of HTSC HVDC system,”
SCDC Project Review Meeting, Palo Alto, CA, 25 July 2008
SCDC cable electrical characteristicsParameter Valueouter radius of inner conductor 17.5 mminner radius of outer conductor 29.5 mmCalculated Quantities Valueinductance, L 104.4 nH/mcapacitance, C 319.6 pF/mcharacteristic impedance, Z0 18.08 Ωpropagation speed, ν 173 x 106 m/s
System Parameter ValueSCDC cable length, l 2000 milescable propagation delay, tDelay 18.6 msControl Variables Valuemaximum voltage ramp rate 40 kV/s
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 4
Transient Oscillations of DC Cables
• Long DC cable system (>1000 km)– the behavior of the converters are affected by the propagation delays introduced by the cables
• the propagation time constant is similar to other cable systems
• with a small frequency‐dependent ac resistance provided by SCDC cables, slower transient signals (<1 kHz) have little attenuated along the cable length
• normal mismatches between the converter impedance and the cable characteristic impedance cause most of the transient signal energy to reflect back into the cable
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 5
Rectifier Terminal-Voltage Control
Inverter Terminal-Current Control Rectifier Terminal-Current Injection Inverter Terminal-Current Injection
Rectifier Terminal-Voltage Level Inverter Terminal-Voltage Level
current ramping to full load at the rate of 5 kA per second
voltage control at the rectifier maintains the dc terminal
voltage at nearly constant valuefor load current changes
voltage level at the inverterterminal exhibits a voltage sag during the ramping up of the
load current
voltage ramping to pre‐chargethe voltage in the SCDC cable
ringing of the current feeding the cable complementary
ringing of the current at the inverter
terminal of the cable
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 6
Ramp Rate Limits for Long Cables• A proper voltage profile is
maintained at the converter with voltage control
• The voltage at a converter with current control sags and swells due to the inductance of the SCDC cable
• The propagation delay and mismatch of the cable’s characteristic impedance with the converter’s impedance results in a decaying oscillation
• The ramp rate of the current affect the magnitudes of the voltage sags, swells, and ringing
Case Peak Idc Greatest Vdc Average VdcRamp Rate Sag Sag
Run #1 1 kA/s -0.38% (79.7 kV) -0.19% (79.85 kV)Run #2 2 kA/s -0.88% (79.3 kV) -0.44% (79.65 kV)Run #3 5 kA/s -2.75% (77.8 kV) -1.38% (78.90 kV)Run #4 10 kA/s -5.50% (75.6 kV) -2.75% (77.80 kV)Run #5 20 kA/s -11.0% (71.2 kV) -5.50% (75.60 kV)
Sags for the 2000-mile SCDC cable
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 7
Impact of Cable Length1000‐mile cable
2000‐mile cable 4000‐mile cable
• Simulation parameters• 80 kV, 10 kA, two‐terminal SCDC cable
• current control terminal: 2 kA / sec ramp rate
• Graphs of voltage ripple
1.13% V_offset2.22% V_ripple
0.302% V_offset0.554% V_ripple
0.583% V_offset1.108% V_ripple
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 8
VSC Model
Single DC pole operationand a SCDC cable with ground return sheath
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 9
1000 km Typical DC Cable
Transient Oscillations
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 10
1000 km Small Resistance DC Cable
Transient Oscillations
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 11
1000 km Near Superconducting DC Cable
Transient Oscillations
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 12
1000 km Near Superconducting DC Cable
Transient Oscillations
Curren
t [kA
]
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 13
Comments
• PSCAD simulations show– that the operation of the VSC converters seem to work adequately as far as the control of voltage is concerned
– however the current transients on the DC line for near superconducting conditions after an AC fault are extremely severe and needs to be dealt with creative solutions and may not be easily achieved
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 14
Control Schemes
• Multi‐terminal systems– extensions of the point‐to‐point system control concepts (based on the notion of control modes)
• voltage regulation mode at one converter station– generally applied to a rectifying converter
• current regulation mode at all other converter stations
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 15
DC Voltage Droop Control
• A distributed voltage regulation scheme for controlling current injections– similar to frequency‐power regulation in ac grids
• a change in voltage used to signal the control system to meet changes in power demand (current injections)
• natural regulation requiring no communications
– performs best on a SCDC mesh or parallel network• each of the nodes reach the same steady‐state voltage level
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 16
Dynamics of Droop Control
• The droop dynamic components– VSC rectifier’s equivalent source impedance– DC capacitors at the terminals of each converter– SCDC cable inductance– SCDC propagation delay for long lines (>1000 km)
• Droop dynamic range– the built‐in droop of a rectifying converter is quite small (e.g., 10’s MW / 0.001 pu of ΔV)
• simplifies the power regulation at inverting converters• large changes in the dc voltage can indicate system problems and trigger load shedding as necessary
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 17
Dynamics with Long SCDC Cables
• Two of the long cable dynamic characteristics cause a voltage differential across the SCDC cable– inductance– propagation delay
• Control scheme must account for the propagation delay of the cable– delay values: 1 ms to 25 ms
November 12 & 13, 2008 Eighth EPRI Superconductivity Conference 18
Two Cable System
• Proposed from a reliability perspective– twin converters and twin cables running in parallel– crossover switches for addressing faulted sections
• From a control perspective:– using both cables simultaneously permits a doubling of the current ramp rates for a specified sag, swell, and ripple requirement
– in the case of a failure, half of the full rated current would need be transferred to the remaining good cable or converter
Copyright © 2008, Praxair Technology, Inc. All rights reserved.8th Annual EPRI Superconductivity Conference
Pulse Tube Cryocooler Refrigeration System for HTS Cables
Praxair, Inc. Greg Henzler
November 13, 2008
28th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Outline
Praxair introduction
Pulse tube cryocooler technology
Columbus, OH cryocooler experience
HTS refrigeration system layout
38th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Praxair at a Glance
A Fortune 300 company
Sales of $9.4 billion in 2007
Largest industrial gas company in North America
Operations in more than 30 countries
One million customers worldwide
28,000 employees
48th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
NorthAmerica
55%
SouthAmerica
17%
Europe14%
Asia8%
Industrial Gases Sales by Region2007 Sales $9.4 billion
Excludes worldwide sales of Praxair Surface Technologies (6% of total sales)
Strategic Global Position
58th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
On-Site Supply Business Model
Plants are located on customer sitesAir separation, H2 and other types of plants
Owned, operated, maintained and updated by PraxairRemote operation and monitoringReliably supply product 24/7 Critical customers include
Hospitals
Chemical plants
Semiconductor fabs
Steel mills
Praxair is viewed as a gas utility by many of our customers
68th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Praxair’s Pulse Tube Cryocoolers
Pressure wave generator (PWG) converts electrical energy into acoustical energy
Coldhead and inertance network convert acoustical energy into refrigeration capability
Process Lines
PWG
Vacuum Container
Coldhead
Coldhead InertanceNetwork
Inertance Tank
Linear Motors with Pistons
78th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Pulse Tube Benefits
No moving parts in cold endNo connecting rods
No wearing partsNo bearings
No oil
Long lifeHigh reliabilityLow maintenanceHigh Carnot efficiencySmall modular footprintLow noise and vibrationEnvironmentally friendly
Key enabler of HTS cable technology!
88th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Linear Motor
Regenerator Pulse Tube
Aftercooler
Reservoir
ImpedanceNetwork
Cold Heat Exchanger
Warm Heat Exchanger
Major components of electrically driven Pulse-tube cryocoolersLinear motor: electrically powered oscillating piston(s)
Aftercooler: water cooled heat exchanger
Regenerator: array of narrow passages - high Cp material
Cold heat exchanger: refrigeration is ‘extracted’ here
Pulse tube
Warm heat exchanger, impedance network, reservoir, oscillating gas
Pulse Tube Basics
98th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
PWG & Cold Head Improvements
2nd generation PWGImproved efficiencyIncreased clearanceExternal thermal management systemNew drift control systemShorter piston stroke length
2nd generation cold headDesign completedHigher cooling capacityImproved heat transferEnhanced regenerator
40 60 80 100 1200
500
1000
1500
2000
2500
3000
Tc, K
Cooling Power, W
1K Unit and Gen-2
1kW
G2
108th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Columbus, OH HTS Cable Project
HTS cable energized 8/8/06~ 20,000 hours of operation
2nd gen. PWG energized 8/20/08
~ 2,000 hours of operation at site
Praxair operates, maintains and monitors refrigeration system
System working well
Termination CryostatRefrigeration System
Chiller
1 kW Cryocooler
PT Cryocoolers
118th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Termination Refrigeration System
85%87%89%91%93%95%97%98%Percent of design capacity per cryocooler =
Cryocooler Shutdown
At full refrigeration demand of5 kW, the cryocoolers operateat 85% of their full capacity.
A loss of 1 cryocooler at full refrigerationdemand results in the remaining cryocoolersoperating at 98% of their full capacity.
128th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Refrigeration System for Long Lengths
Cryocoolers at the substations only
GORETURNGO
RETURN
cooling channels
cryostat
cable
steel pipe
138th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Cooling System Key Components
Pressure Wave Generator (PWG)Two opposing pistons on linear motors
ColdheadHeat exchangers and regeneratorNo moving parts
Water chillerPackaged unit
Cold boxCryo valves, piping, pumps etc.
ControlsVFDTemperature, pressure, vibration etc.
Majority of components are existing technology and readily available.
148th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Benefits of Independent Cryocoolers
Each cryocooler is operated by a single PWGIf a motor fails, then only one cryocooler failsEach cryocooler acts independentlyLeads to overall higher reliabilityManage redundancy on a smaller scaleMore turndown flexibility
158th Annual EPRI Superconductivity Conference Copyright © 2008, Praxair Technology, Inc. All rights reserved.
Conclusions
Praxair reliably supplies product for critical applications in diverse industries
Pulse tube cryocoolers are a key enabler for HTS cable applications
Praxair continues to have significant success with pulse tube cryocooler technology
1 Managed by UT-Battellefor the Department of Energy
Bill SchwenterlyOak Ridge National Laboratory
Ed PlevaWaukesha Electric Systems
Alan WolskyArgonne National Laboratory
November 13, 20088th EPRI Superconductivity
Conference
Cost and Performance Comparisons Between HTS And Conventional Utility Power
Transformers
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OUTLINEDesign assumptions
Overview of design spreadsheet
Capital and Operating Cost Comparison
Efficiency Comparison
Weight and Dimension Comparison
Other Design Issues
Summary of Requirements
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HTS Unit Design Summary25-MVA rating; 115 kV / 13.09 kV; 72 A / 1103 AYBCO winding in pressurized, subcooled nitrogen bath
HV– Disc, 10 turns/discLV– Transposed screw, 8 wide or 16 narrow tapes in parallelWrapped insulation on conductorsCo-wound 1-mm copper
Pressurized bath is coupled to cryocooler by cooling shell.
Air-cooled compressorsComposite dewar
Metal dewar would form a shorted turn around core.Core in air
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Conventional vs. HTS Unit Ratings Comparison
Conventional Unit15/20/25-MVA ratings with no fans/1-stage fans/2-stages fans.30 minute operation at 50 MVA with increasing winding temperature.
HTS UnitCryocoolers are sized for 25-MVA heat load.HTS is sized for 50-MVA load with Ipeak < Ic.15/20/25-MVA ratings with cryocoolers cycled to match heat loads at lower ratings.30 minute operation at 50 MVA with liquid nitrogen boiloff.Current leads are sized for 125% of 25-MVA current.Maximum current lead temperature rises to 120°C at 50 MVA with increased heat load.
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Transformer SchematicBushings
Cryocooler
Shield
CoreWinding Foam
Composite CoilDewar
CoolingShell
PressurizedSubcooledNitrogen
RemovableTop Plate
Unit is surrounded by weather enclosure in place of oil tank.
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Single-Phase Transformer Concept
Core
Composite Dewar
AL-300 Cryocooler
138-kV Bushing
Winding PackCooling Shell
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Common Dewar for 3-Phase Unit
Stainless outer jacket
Composite top & bottom plates
Composite core limb jackets and winding vessels
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Overview of HTS Unit Design Spreadsheet
Inputs:Ratings and voltages; overload factor5 different volt/turn values can be specifiedConductor dimensionsWinding geometry– disc or layer; number of layers or disc turnsMaterials properties– Ic, cost, densityWall thickness for coil structure and dewarsInsulation thickness and voltage standoff distancesRefrigerator dimensions, weight, input power, cost
Outputs:Capital and operating costsWinding, dewar, core, and enclosure dimensionsWeights-conductor, core, dewarLength of conductorLead and ac loss heat loads (Rhyner’s equations for ac losses)Room temperature input loss power% Fault impedance
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1010 Managed by UT-Battellefor the Department of Energy
15-MVA 30-Year Capital and Operating Costs
Assumptions: $50/kA-m HTS, 350 A/cm, 0.6 cm width, 70-K Toper$8.80/kg copper, $4.20/kg steel 120 V/turnLoad losses– $1250/kW No-load losses– $2500/kW
Item HTS Conventional
Selling Price $680 K $458K
No-Load Loss $84 K, 34 kW $35 K, 14 kW
Load Loss $4K, 3.3 kW $58K, 46 kW
TOTAL $768 K $551 K
Oil Containment ---- $30 K
Fire Suppression ---- $100 K
Refr. Maintenance (2 AL-600) $106 K ----
GRAND TOTAL $874 K $681 K
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High cost of conductor forces minimum in lifetime cost to high volt/turn values.
V/n gives required number of turns in a phase.
V/n = απRcore2
α = 4.44 f Bcore
Lcond = 2πRcoren = 2V/αRcore
Thus, larger core diameter reduces conductor length.
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15- and 25-MVA EfficiencyAssumptions: Refrigerator COP– 27 W/W.
2 Cryomech AL-600 refrigerators, ea. 560 W at 70 K, 15 kW input power.HTS and Lead losses are refrigerator input power.
Item HTS Conventional
Load 15 MVA 25 MVA 15 MVA 25 MVA
Core Loss 23 kW 14 kW
AC Loss 2.9 kW 13.1 kW ----
Lead Loss 7.4 kW 8.8 kW ----
Copper Loss ---- 46 kW 131 kW
TOTAL LOSS 33.3 kW 44.9 kW 60 kW 145 kW
EFFICIENCY 99.8 % 99.8 % 99.6 % 99.4 %
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15-MVA Dimensions and WeightsAssumptions: 0.3 m side and 0.1 m top/bottom enclosure clearances
Item HTS Conventional
Length 3.75 m including compressors 3.02 m
Width 1.65 m 3.33 m including radiators
Height 4.22 m including bushings 4.92 m including bushings
Core weight 16.4 t 9.1 t
Total weight 24.0 t 39.9 t
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What if conductor cost is lowered?Minimum in total cost moves down and to left as conductor cost falls.
Capital cost approaches conventional at $10/kA-m.
Copper– ~$25/kA/m in conventional unit at 3A/mm2.Capital costs shown are atminimum total lifetime cost.
Refrigerator cost reduction ($109K in present design) would also help cost comparison.
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15-MVA 30-Year Capital and Operating Costs
Assumptions: $20/kA-m HTS, 350 A/cm, 0.6 cm width, 70-K Toper$8.80/kg copper, $4.20/kg steel 70 V/turnLoad losses– $1250/kW No-load losses– $2500/kWRefrigerator cost reduced by half
Item HTS Conventional
Selling Price $478 K $458K
No-Load Loss $60 K, 24 kW $35 K, 14 kW
Load Loss $5K, 4 kW $58K, 46 kW
TOTAL $543 K $551 K
Oil Containment ---- $30 K
Fire Suppression ---- $100 K
Refr. Maintenance (2 AL-600) $106 K ----
GRAND TOTAL $649 K $681 K
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Other Design Issues– Fault HandlingIEEE/ANSI Standards specify a 2-sec total fault duration without overheating.Extra copper is needed for fault handling.
2-sec requirement leads to large fraction of a conventional unit’s Cu!1 mm of copper is adequate for 1/2-sec 10X fault.
Copper cannot be co-insulated with HTS tapein advance because the inner conductorbuckles during winding.
HTS tape is too fragile to wind with high-voltageinsulation by itself.Winding on insulation as coil is wound is not practical,especially for multiple conductors in LV winding.
Need copper laminated or plated on both sides of the HTS tape,so that the HTS is on the neutral axis.This would provide a robust conductor that could be insulated ona high-speed machine.
HTS
Copper
Insulation
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Other Design Issues– Layer Build, Core,AC Losses
Designs with ~20-turn discs are desirable.Core limbs >2 m high are flexible and hard to handle in shop.Smaller core with shorter limbs and lower losses is possible with more turns in discs.At constant window area,h/w ratio of β = 4/3 minimizes core loss.
Window area Aw = hw = βw2 = h2/βCore volume Vcore = Acore[3h + 2(2w+3Dcore)]Vcore = Acore[3√ Awβ + 4 √ Aw/β + 6Dcore]Derivative = 0 with β = 4/3.
BUT-- more turns on a disc raises field on HTS conductor on inner turns and increases ac loss.
HTS loss reduction needed– striations, nano-particles, etc.
w
h
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SUMMARY– For a competitive HTS Transformer:
We need HTS tape cost near $20/kA-m. *(Not including extra Cu)
We need HTS tape with 1/2 mm or more of copper laminated or plated on each side.
We need HTS tape with ac loss reduction features such as striations or nanoparticles.
We need reduced cryogenic refrigeration costs.
With higher no-load losses and lower load losses than a conventional unit, an HTS transformer is most appropriate in a base load application where it is loaded most of the time.