24 overhead lines and cables
TRANSCRIPT
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Room 6.2
.Wednesday, 14th September(11.00 - 12.45)
Rpt: Marco Marelli
241 HV submarine cables for renewable offshore energy - G. Dell Anna,P. Maioli, A. Micheletti, E. Zaccone
242 Past experience and future trends with compact lines to solve theright-of-way issue - K.O. Papailiou, F. Schmuck
-
AC/DC hybrid line with regard to audible noise - U. Straumann, C.M.Franck
au curren m ng power ca es or m ga on o au eve s ntightly interconnected systems - K. Howells, D. Folts, J. Mccall, J. Maguire
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HV Submarine Cables For
Renewable Offshore Energy
Gaia Dell Anna, Prysmian Power Link,
Andrea Micheletti, Prysmian Power Link,Ernesto Zaccone, Prysmian Power Link,
Paolo Maioli, Prysmian S.p.A.
CIGRE Bologna 2011
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The Offshore power generation
The recent years have shown a large
generation especially in the European northern
Sea areas
The location of these large off shore wind farms
and requested the adoption of submarine cableconnections that are the unique possiblesolution
epen ng on e s ance an e power o etransmitted both ad hoc HVAC and/or HVDCsolutions have been ado ted.
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Ambitious European Projects
Moreover, a so-called" "is proposed for integratingoffshore wind ener in theNorth and Baltic Seas into afuture EU internal electricity
market.
SCOTLAND is also
mentioned as a key region
various renewable energysources accountin for u to
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68 GW by 2050.
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Characteristics of HVAC Cables
Cable structure description
Armoring Losses IEC 60287vs laboratory experience
capabili ty test experience
Mechanical performance
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Typical HVAC submarine Cable
1) Copper conductors
3) XLPE extruded insulation
4) Semiconducting insulation screen
5) Swelling tapes
6) Lead alloy sheath
o yet y ene ac et
8) Polypropylene fillers
9 Pol ro lene bindin
10) Polypropylene string bedding
11) Galvanized steel wire armour
12) Polypropylene string serving
13) Fiber optical unit
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Typical HVDC submarine Cable
1) Conductor
3) Extruded insulation
4) Semiconducting insulation screen
and Swelling tapes
5) Lead alloy sheath
6) Polyethylene jacket7) Polypropylene string bedding
8) Galvanized steel wire armour
9) Polypropylene string serving
Typical diameter: 90 to 120 mm
CIGRE Bologna 2011
THE VSC COVERSION TECHNOLOGY;TRADITIONAL MI CABLES ARE ALSO AVAILABLE IF
NECESSARY
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Cable testing
Magnetic field measurement
Very low EMF emissions
Phase resistance of HV tricore cable.-
4,5E-05
, -
/m
]
3,5E-05
4,0E-05
e
resistance
[Oh Pb closed wi th armouring
Pb closed no armouringMagnetic field measurement
3,0E-05
Phas
Very low EMF emissions
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0 200 400 600 800 1000 1200 1400 1600 1800
Current [A]
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Cable testing
Mechanical testing in laboratory
Magnetic field of 132 kV tricore cable: current 400 A.
1000,00
measured wi th armourning
computed parallel
10,00
100,00
ld[microTesla]
computed helix
Magnetic field measurement
0,10
,
Magneticfie
Very low EMF emissions
CIGRE Bologna 2011
,
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6 1,8 2,0 2,2 2,4 2,6 2,8 3,0
Distance from cable axis [m]
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HVAC or HVDC ?
HVAC is more practical and simple, but may have some limitation in the lengthand transmissible power.
HVDC require the conversion stations; the VSC technology converters allow the
installation on offshore platforms and advantages in the management andregulation of the transmissible load.
The adoption of the solution isevaluated case by case, on atechnical and economicalevaluation.
As a rule of thumb the ran e ofconvenience of HVAC Vs HVDC can
be summarized by this graph.
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Greater Gabbard
One of the largest offshore wind farms
Customer:
InnerGabbard
Fluor Ltd
Project ownership:
site
NPower
Project Scope:
Main offshore
section 3 x 132kV
Cables 800mm2
(each 47km)
Cable to connect 2platforms1 x 132kV Cable800mm2(19km)
504 MW with 140 wind turbinegenerators
Gallopersite
160 km 3 core 800 mm2 CuXLPE Pb SWA Submarine cable
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Typical Layout of an Offshore Wind Farm
Transmission Grid
HV station
HVAC or HVDC cableMV Cables 20 or 30 kV
contribution
-transformer platform
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BorWin 2
400 km cable, 300 kV, 800MW HVDCGrid Connection of offshore wind farms
Route Length:
76.4 km HVDC Onshore Route (150 km cable)
123.4 km HVDC Offshore Route (246.8 km cable)
2x11.4 km & 2x28 km HVAC Offshore Route (79.8 km cable)
ower a ng o age eve :
800 MW @ 300 kV
155 kV AC
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HelWin1
HelWin1 260 km HVDC cable, 250 kV, 576 MW
Route Length:
45.5 km HVDC Onshore Route (91 km cable)
85 km HVDC Offshore Route (170 km cable)
x . m s ore ou e . m ca e
Options: 2 x 7.6 km HVAC Route
Power Rating / DC Voltage Level:
576 MW @ 250 kV
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SylWin1 & HelWin2
SylWin1 410 km cable
320 kV, 900 MW HVDC
HelWin2 260 km cable
320 kV, 690 MW HVDC
Route Length:
45.5 km HVDC Onshore Route (91 km cable)
159 km HVDC Offshore Route (318 km cable)
Route Length:
46 km HVDC Onshore Route (92 km cable) 85 km HVDC Offshore Route (170 km cable)
x . m s ore ou e . m ca e Options: 2 x 40km & 2 x 35km HVAC Route
Power Rating / DC Voltage Level:
900 MW @ 320 kV
2x8 km HVAC Offshore Route (16 km cable)
Power Rating / DC Voltage Level:
690 MW @ 320 kV
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Alpha Ventus
First Major German Offshore Wind farm
E.ON Netz Offshore
Cable scope:66 km 110 kV 3 core 240 mm2 CuXLPE Pb SWA cable and accessories
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Thanet Project
Customer:Thanet Offshore Wind Ltd
Cables:55 km 132 KV 3 Core 630/1000 mm2
72 km 33 KV 3 Core 95 300 400 mm2
140000
160000
180000
G1F1E1
D1
C1
B1
Line 8
Line 7
80000
100000
120000
A1
G11
Line 1
Line 2
Line 3
Line 10
Line 9
20000
40000
60000
A12 D17C15B14
E17
F14Line 4
Line 5
Line 6
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0
0 100000 200000 300000 400000 500000 600000 700000
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an you or your a en on
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
Paper 242
RIGHTOF
WAY
ISSUE
by
.
.
.
PFISTERERHOLDINGAG PFISTERERSEFAGAG
. . . .
UniversityofBologna,FacultyofEngineering September13th 15th,2011
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
CompactionLine
means
50m 9.6m
UniversityofBologna,FacultyofEngineering September13th 15th,2011January2006IdeaforCompaction
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
easons
or
ompact
ne
rrangements
Reduction of total line costs.
Right of Way (ROW).
Redundancy due to bracing longrod.
Reduction of influence of the electroma netic field.
aesthetic-visual impact, pleasing to public.
in service since the 80ies. e.g. nUSA,Ita yan Greece
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
Prosan
Cons
o
Compact
Lines
Pros
Cost savings for tower and foundation construction.
Aesthetically pleasing.
Reduced EMV on ground level. Higher power transfer capacity because of lower surge
impedance.
Fail-safe redundancy because of the use of twoinsulators in the case of braced line posts.
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
Prosan
Cons
o
Compact
Lines
Cons
Increased corona level because of shorter distances
Shorter span lengths (if no phase spacers are used)
More demanding conductor stringing process Maintenance issues, especially live-line-work
Mechanical stability problems.
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
e
w ssexper ence
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Ci 2011 B l S i Th El i P S f h F
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
e
w ssexper ence
420kV
com act
420kV
traditional
Steellatticetowerof125kV19m
lineandSwisscompacttower
for400kV/132kVlineaswellas125kV
8.6m
9m
UniversityofBologna,FacultyofEngineering September13th 15th,2011
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Real-life a earance of Profiles o timized for mechanical
unique compact tower strength versus material use
Ci 2011 B l S i Th El t i P S t f th F t
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
ons era ons compactconventional
UniversityofBologna,FacultyofEngineering September13th 15th,2011Simulation
for
current
of
1000
A
and
at
1
meter
above
ground
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
xamp eo
w ss
tra t on
van age e erer
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
T eSwiss
experience
Combinationofinnovativeconcepts
CarbonFiberReinforcement
+lowerweight
+ no corossion
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
So utionso
Con uctor
Attac ment
Sus ended
Multifunctional
solutionwitha
plasticbumper
rigidattachmentrigidattachment
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
equ remen s
or
es ngMechanicalDesign
FEMSimulation,especiall FullScaleTesting
ForceProbe
ResultingForce
Angle
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
equ remen s
or
es ngElectricalDesign
FEM(BEM)Simulation,especiall FullScaleTesting
PhaseB PhaseB
PhaseC PhaseA
UniversityofBologna,FacultyofEngineering September13th 15th,2011
Cigr 2011 Bologna Symposium The Electric Power Systemof the Future
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Cigr 2011 Bologna Symposium The Electric Power System of the Future
Summary
-solutions to solve right-of-way constraints and to provide
a technical solution to reduce electromagnetic field onground.
They are a very attractive solution when upgrading an
existing transmission system, e. g. from (123 kV as inCH) 245 kV to 420 kV.
They have been introduced for voltage levels up to 420kV so far, further developments for 525 kV and if possible
.
A full scale mechanical and electrical testing is highly-
UniversityofBologna,FacultyofEngineering September13th 15th,2011.
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g g y p y
esponseto
uest ons
+
solution in comparison to cable or gas-insulated line
(GIL). Due to the reduced mechanical load to the pole ortower, very aesthetic solutions can be introduced.
It is recognized to be the only solution when upgrading an
existing transmission system, e. g. from (123 kV as inCH) 245 kV to 420 kV.
The existing standard IEC 61952 provides general rulesfor composite post insulators, however the solutions are
-conditions and locally applicable laws.
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Discussion of Converting a Double-Circuit AC Overhead
Line to an AC/DC Hybrid Line with Regard to Audible Noise
. , . .High Voltage Laboratory, ETH Zrich
Cigr-Symposium, Bologna, September 13-15, 2011
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 2
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Problem
RenewablesCapacity increase of transmission
Contents of the presentation
s nee e
No new transmission corridors
1)Interaction Between Circuits in aHybrid Line
alternatives to increase capacitieswithin existing ROWs e. .: convertin AC to DC
Investigated Conversions
3)Audible Noise Characteristics of
Existing lines
s
4)Tower Geometries, CalculationMethods
(limiting land use):multi-circuit lines
5)Calculation Results
lines
U. Straumann and C.M. Franck
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 3
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1. Interaction Between Circuits in a Hybrid Line
Coupling between AC/DCsurface gradients
capacitive and magnetic coupling (AC-current in the DC-poles) ion current from coronating DC- pole collected by AC phases (DC--
Technical consequence
overvoltages of the DC circuit is increased in hybrid environmentunknown consequence on requirements on insulators in a hybrid
U. Straumann and C.M. Franck
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 4
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2. Investigated Conversion
Original line400 kV AC double circuit line
Conductors and their thermalratings
Conversion
Replacing one circuit with a500 kV DC circuit
Transmission capacity
1)Corridor: 160 %
U. Straumann and C.M. Franck
2)Single circuit: 220 %
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 5
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3. Audible Noise Characteristics of OHLs
Corona leads toIon currents
DCOnly broadband crackling &
a o n er erenceLosses
Audible noises (AN)
ss ng no seStrongest in dry weather
AC
Broadband and tonal noise (2f)DC vs. AC
Example (EPRI)
tonall
crackling
ise
lev
100 HzNo
~ (1-10) kHz
A-wei htin
U. Straumann and C.M. Franck
Frequency [HVDC Transmission Line Reference Book]
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 6
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4. Tower Geometries, Calculation Methods
Geometries LiteratureDC ions do not affect the AC
corona significantlyAC and DC corona may be
affected by superimposed fields,but: Emission may be calculatedby combining the formulas forure AC- and DC-lines
Tonal emission is notcommented
Calculation of audible noise
Formulas from EPRI
Ground wire: 22.4 mmAC-conductor: 27.0 mm
DC noise: HVDC TransmissionLine Reference Book
AC: Transmission Line
U. Straumann and C.M. Franck
-con uc or: . mm Reference Book
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 7
5 C l l ti R lt
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5. Calculation Results
HybridOriginal (2 x AC 400 kV) fair (DC)
fair rev. DC
40[d
B(A)]
[d
B(A)]
40
foul weather (AC)
3
35
velL
eq
circuit 1 velL
eq
30
35
- -
25noise
le circuit 2
totalnoisel
25
-100 -50 0 50 100
lateral distance from line axis [m] lateral distance from line axis [m]
AC AC DCAC
U. Straumann and C.M. Franck
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 8
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Conclusion
1) Increase of transmission capacity by the investigated conversion isquite considerable
2) Even though a larger coupling between the AC and DC circuits may
be disadvanta eous in some technical res ects intermixin the ACphases and DC poles on both sides of the tower reduces the surfacegradients and the AN levels in the investigated examples.
3) Polarity reversal may be accompanied by a remarkable change of DCAN levels.
Outlook
Quantification of space charges (ion flow fields):determining electric fields
U. Straumann and C.M. Franck
evoking the DC-current in the AC-phases
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 9
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U. Straumann and C.M. Franck
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 10
2 Origin of the Audible Noises
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2. Origin of the Audible Noises
PD-patternCorona-discharge
roa an omponen ,
on uc or:ESurface: 20.9 kVpeak/cm
Rain: 8 mm/h
conductor
rotrusion(water drop) 20
]
Strong pulsative dischargesoccur at the ositivel stressed
10itude
[n
electrode
Ampl
AC: Only positive half-waveDC: Only positive pole
0 180 360Phase []
U. Straumann and C.M. Franck
Cigr-Symposium, Bologna, September 13-15, 2011 Slide 11
4 Tower geometries calculation methods
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4. Tower geometries, calculation methods
Geometries LiteratureDC ions do not affect the AC
corona significantlyAC and DC corona is affected by
the superimposed fields Emission may be calculated bycombining the formulas forure AC- and DC-lines
Tonal emission is notcommented
Calculation of audible noise
Formulas from EPRI
Ground wire: 22.4 mmAC-conductor: 27.0 mm
DC noise: HVDC TransmissionLine Reference Book
AC: Transmission Line
U. Straumann and C.M. Franck
-con uc or: . mm Reference Book
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Fault Current Limiting Power Cables for Mitigation of FaultLevels in Ti htl Interconnected S stems
Kyle Howells Doug Folts J ack McCall J im MaguireAmerican Superconductor Corporation
CIGRE Symposium
Electric Power System of the Future
Bologna, 13-15 September 2011
Paper 244
1
F lt C t B i
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Fault Current Basics
The maximum
magnitude offault current is a X/R Ratio Typical Systems
for both AC and
DC components
High, 14 Transmission Systems
Industrial Feeders
-
Higher Z reducesfaults at the
,8 14 Large Distribution S/S
Long Feeders
2
expense of
higher losses
,
Th R l f X/R
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The Role of X/R
The maximum The X/R ratio affectsthe duration of the DC
affected by the fault
closing angle
offset
Higher X/R will have
X/R neither helps norhurts in these terms
slower decay
Adding R damps offset
3
S t I d d F lt
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S stem Im edance and Faults
Adding X to system impedance- Lowers overall fault magnitude
- Increases losses
- Increases DC offset decay time
- Negative impact to system stability
Adding only R to system impedance-
- Increases losses
-
- Positive impact to system stability
4
Adding resistance during faults is preferable
S d t F lt C t Li it
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Su erconductor Fault Current Limiters
Superconductor FCLs fall into two categories:
Inductive- These often take the form of a saturable core reactor
field
-Uses superconductors highlynon-linear resistive impedance during
ResistiveBypass Element
quenc o res s ve y m curren an
- To bypass the current into a
arallel b ass elementNon-linear
superconductorelement
5
Key HTS Cable ELECTRICAL Characteristics
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y
Ver hi h ower transfer ca abilit com ared toconventional cables solves many siting problems
ery ow mpe ance re uces oa ng on para e nesand equipment
Minimal magnetic field and elimination of heatsimplifies placement concerns, minimizes right-of-way,an s easy on e env ronmen
O tional HTS cables with fault current mana ementcapabilities eliminate need to upgrade existing equipmentHTS Cables offer unique capabili ties
Power Transfer Equivalency ofSuperconductor Cables
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Superconductor Cables
230kV XLPE
HTS
,Power
- Greatly increased
ower transfer ca acit
69kV XLPE
XLPE
HTS
at any voltage level
Same Power, LowerVoltage
34.5kV
XLPE
XLPE
HTS
HTS- New MV versus HV
Siting Opportuni ty MV Transmission
0 200 400 600 800 1000
.
Power Transfer Capabili ty - 3-phase MVA
ea or ROW sparseenvironments
* No XLPE cable de-rating factors applied.Superconductor rating based on conventional 4000A breaker rating
Superconductor cables provide transmission-level power transfer at medium voltage
Superconductor Example:138 kV 575MW Capacity
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138 kV, 575MW Capacity
200 ft ROW Self contained thermal
envelope No thermal de-ratin
Self contained thermalenvelope No thermal de-ratin
Minimal magnetic field
No parallel line de-rating
Minimal magnetic field
No parallel line de-rating
Longer practicaldistance
Longer practical
distance
4 ft ROW
Superconductor Cables Simplify Placement and Offer New
Options to Siting Lines
Fault Current Limiting Cable Operation
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high resistance layer
Load
zero resistance superconductor layer
Superconductor wire has zero resistance up to
Current
high resistance layer
the critical current
switched high resistance superconductor layer
au
Current
SimplifiedView of
Supercond
uctor wire
Superconductor wire instantly introduces highresistance above the critical current
Immediate limi tation of fault current magnitudes
Insertion of resistance decreases X/R and faultasymmetry
The switching of conductive state is a function of the
superconductor material itself and requires no external control
Current Division in Superconductor FCL CableDurin Quench
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Durin Quench
10
FCL Cable O erational Characteristics
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FCL Cable O erational Characteristics
Fast Res onse- Millisecond
operation
First Peak
RMS Limiting Photo: Courtesy U.S. Dept. of Energy,Oak Ridge National Laboratory- es s ance u s as au
progresses
- Lowers X/R ratio, reducing DC
offset
A Com lex S stem Exam le
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A Com lex S stem Exam le
Paralleling 3 substations-
- Improves load servingcapacity
esu s n g au currencontributions
FCL method re uired
Superconductor Cables Equivalent X/R Cables
17% additionalfault current
re uc on ueto phase shifteffect of
12
cable
Paralleling Urban BusesParalleling Urban Buses
Servin Additional LoadServin Additional Load
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Servin Additional LoadServin Additional Load
HTS Interconnected Substation Loading IncreaseHTS Interconnected Substation Loading Increase apa y; n- r er a
140%
160%
180%
ad
Capabilit y; n -1 Criteria
80%
90%
100%
d
60%
80%
100%
120%
Increas
edLo
Capab
ility
3 XFRMR
4 XFRMR5 XFRMR
30%
40%
50%
60%
70%
ncrease
dLo
Capab
ility
3 XFRMR
4 XFRMR
5 XFRMR
0%
20%
40%
2 3 4 5
Number of Interconnected Substations
%
0%
10%
20%
2 3 4 5
%I
Interconnecting Substations significantly increases load serving capabili ty*
* Theoretical limits
Summar
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Summar
inductance
- 3-10x the normal MVA capacity of XLPE cables
- Simplified right-of-way and placement requirements
- No external EMF
Resistive fault current limiting can be added tosuperconductor cables
- Provides first cycle current limiting
-Lowers X/R, reducing DC offset
- Provides system damping
-
14