HTS insert magnet design: Stack Cable Johnny Himbele, Arnaud Badel , Pascal Tixador
ESAS School 2011 SMES Tixador - Prizztech Oy · Ni-Cd batteries Long dura. flywh ... – Relay...
Transcript of ESAS School 2011 SMES Tixador - Prizztech Oy · Ni-Cd batteries Long dura. flywh ... – Relay...
SMES Pascal Tixador
Grenoble INP - Institut Néel / G2Elab
Some materials provided by C. Luongo
European Summer School on Superconductivity 2011
SMESSuperconducting
MagneticEnergyStorage
3 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Storage syst. characteristics
! Energy density (volume - mass)
! Power density / discharge duration
! Cost (/kWh - /kW) investment & running
! Operation security / fail characteristic
! Life time / cycles number
! State of the technology
– demonstration / emerging / mature
! Environnemental considerations
Introduction
4 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Comparisons, orders of magnitude
! 1 kg coal 8 kWh! 1 kg wood 4 kWh! 1 kg oil 10 - 12 kWh! 1 kg natural gas 10 - 14 kWh! 1 kg enriched uranium 600 000 kWh! 1 kg of water - 1000 m fall 0.003 kWh! 1 kg Pb battery 0.03 kWh! 1 kg lithium battery 0.2 kWh
(1 kWh : kinetic energy of a 10 ton truck at 100 km/h)
Introduction
5 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy storage in a coil
coilL, R
R = 0 => ! infinite => energy stored and available
Rare mean of electricity direct energy storageSuperconductors indispensable
!
W =1
2LI2
=Woe
"2t
#
Device: SMES (Superconducting Magnetic Energy Storage)
!
I .C. : t = 0 ; I = Io" I = I
oe
#t
$ $ =L
R
%
& ' (
) *
Introduction
6 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES: dual of capacitor
I I
V V VoltageCapacitor
CurrentSMES
SourceDischargeStorage
!
1
2L I
2
!
1
2C V
2
Introduction
7 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
First SC device in a grid
BPA SMES on the grid installed in 1979(transmission stabilization, low frequency power oscillation damping)
Pmax 10 MWf 0.35 HzWmax 30 MJWexch 9.1 MJIo - Vo 5 kA - 2.2 kVØmagnet 2.7 m
One year operation. Cryogenic problems andother solution to damp the oscillations.
Introduction
SMES
• Performances• Applications• Limits
9 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy and power densities
Ragone chart:
Performance
comparison
of storing
devices
Performances
0,001
0,01
0,1
1
10
100
1000
104
105
0,01 0,1 1 10 100 1000Mass
spe
cific
power
(kW
/kg)
Mass specific energy (Wh/kg)
Super
capacitor
Batteries
Dielect
ric
capa
cito
r
SMES
Batteries
Fly-
wheel
10 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES application
0,001
0,01
0,1
1
10
100
1000
104
105
0,01 0,1 1 10 100 1000Mass
spe
cific
power
(kW
/kg)
Mass specific energy (Wh/kg)
Super
capacitors
Batteries
Dielect
ric
capa
cito
rs
SMES
Batteries
Performances
Disch
arg
ing
time
Power
SMESHigh power
supercaps
Hours
Seconds
MinutesHigh power flywheels
Ni-Cd batteries
Lead-acid batteries
Lon
g d
ura
. fl
yw
h.
Li-ion batteries
NaS batteriesHigh energy
supercaps
Pumped
hydro
CAES
Metal-air
batteriesFlow batteries
100 MW100 kW1 kW
www.electricitystorage.org
11 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy & power limits
Metallic structure with 100 MPa: 12.5 kJ/kg (3.5 Wh/kg)
Metallic structure limit: 30 - 50 kJ/kg (present: 14 kJ/kg)
Composite structure limit (theoretical): 150 kJ/kg
Mechanics: very important for SMES
• Energy
!
W
Vol"1
2
B2
µo
" Magnetic flux density
Performances
" Mechanical stresses
!
Volstructure
"# (Viriel th)
!
" = J B R (solenoid)[ ]
B = 10 T => 40 MJ/m3 (11 kWh/m3)
12 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy limit: viriel theorem
!
W "#
d(Masstraction $Masscompression )
Performances
Infinite solenoid:
!
B = µoJ e
&
" = JB
2R
!
W
Vol=
W
2" Re h=
1
2 µo
B2" R
2h
2" Re h=
B
2 µo
B R
2e=J e
2
B R
2e=#
2
Same expression for flywheel (conversion machine required).
With compression stresses:
!
W
Vol="
3
R
e
h
13 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy limit: viriel theorem
!
W "#
dMass
traction
Mechanics: very important for SMES
Performances
Very important to combine functions:Mechanical support & current transport
Ultimate limit:
Reduce mass: protection may become an issue
Rather low limit
14 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy & power limits
• Power (VI)" Voltage & current
# Good electric isolation
• He gas bad dielectrics
# High current conductor0,001
0,01
0,1
1
10
100
1000
104
105
0,01 0,1 1 10 100 1000
Mass
spe
cific
power
(kW
/kg)
Mass specific energy (Wh/kg)
SMES
Super-
capacitors
Batteries
Dielect
ric
capa
cito
rs
" Eddy current losses
# Cryostat
# Conductor (coupling losses)
Performances
15 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Summary: SMES
! High power density & large energy density
– Directly usable current source
! Quick response time
! Number of charge-discharge cycle very high (infinite)
! Static system / low maintenance
! Specific application of superconductivity
! Conversion efficiency may be high (> 97 %)
! «!Correct!» from environmental point of view
! Security of operation
! High costs (cryogenics - superconductor)
! Losses in storage mode (but not really a storage system!)
Performances
SMES
• Examples• Applications
17 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SC magnets: examples
ITER toroid41 GJ; 5600 tons
CMS solenoid2.6 GJ; 225 tons
11 kJ/kg(1.14 ton oil, 19 g U)
18 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES main applications
! UPS, voltage-power quality & reliability– Protection against voltage drop and sags– Relay before the starting of a generating unit
! FACTS (Flexible AC Transmission System)– Supply/absorption active & reactive powers– Grid stability improvement– Transmission voltage regulation
! Pulse power supply– Electric guns– Electromagnetic launchers
! Large energy storage– Daily load leveling– Spinning reserve / frequency control
19 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Energy storage for the grid
! Large energy storage– Daily load levelling (1000 MW / 5000 MWh)
– Spinning reserve (10-100 MVA / 5-50 MWh)
– Frequency control (10-100 MVA / 10-500 kWh)
– Transient stability (100 MVA / 50 kWh)
! Improvement of power quality
Reduction of voltage disturbances– Voltage sag smoothing (1-10 MVA / 1-10 kWh)
– Flicker mitigation (1-10 MVA / 1-10 kWh)
Grids in general requires more reactive than active power
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2011 ESASSummer school
SMES for UPS or FACTS
ConverterEnergy
exchanges
Transformer
Control
Electric grid (AC)
SuperconductingMagnet (DC)Cryostat
Powerconditioning
system
Interface
grid/magnet
!
1
2L I
2
=
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2011 ESASSummer school
Pulse power source
ControlPrimarysource
Switch
LOAD
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2011 ESASSummer school
Electromagnetic launcher/catapult
Performances
Electric railgun:=> Oversteps the speed reached by chemical methods
IEEE Trans. onMagnetics,vol.!43, 2007
Load 4 kgDiameter 80 mmLength 22 mWkinetic 9,1 MJWelectric 27.3 MJ"max 13200 g"t 21 ms
Airplanes launcher:Electric (/steam) catapult
! Linear electric motor
! pulse power supply
SMES
The 4 sub-systems
24 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES - 4 sub-systems
• SC magnet with its supporting structure
• Cryogenic system
• Cryostat, vacuum pumps, cryocooler, …
• Power conditioning system
• AC/DC conversion (inverter + chopper)
• Control system
• Electronics, cryogenics, magnet protection, …
Sub-systems
SMES
Magnet• Topology• Mechanics
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2011 ESASSummer school
SMES - magnet design
Magnet design
• Leak magnetic field
• Mechanical support
• Superconductor quantity
• AC losses
• Protection
Magnet
27 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
I
ToroidSolenoid
Magnet topologies
Magnet
28 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES magnet topology
Simple structure Stray fieldSOLENOID High stored energy Large coils
per conductor unit
TOROID Low stray fields Lower stored energy Smaller unit coils per conductor unit
Mechanical structure
Mechanics: very importantSMES magnets subject to strong Lorentz forces,
If not properly handled, rated performances not achieved.
Magnet
29 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Solenoid: stray field reduction
Stray field reduction: - active shielding - suitable configuration
Main solenoid
Compensating coils
Superconductor volume # x 2
Magnet
30 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Improved solenoids
Hexagonal arrangement
• modular design
• Reduced stray field
• “small” elementary coil
• solenoid simplicity
(force holding)
Magnet
31 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Mechanics - solenoid
Flux lines and electromagnetic forces(M. Wilson)
I
Independent turnsDependent turns
-100
-50
0
50
100
150 200 250 300 350 400 450
Pancakes 13 - 14
!" (MPa)
!'" (MPa)
Hoo
p st
ress
(M
Pa)
r (mm)
!
" = J B R (independant turns)
Magnet
32 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Mechanics - toroid
Flux lines and electromagnetic forces(A. Devred)
Toroid coils submittedto a net large radialforce towards thecentral axis in additionto the transverse andlongitudinal forces.
+ pb in case of aquench
Magnet
SMES
AC losses
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2011 ESASSummer school
AC losses
AC losses + cryostat losses (eddy currents)
" Reduce the useful energy
" Increase the heat load for the cryocooler
" Increase the temperature: limits performances
Low AC loss conductor (LTS)
SMES
Magnet stability & protection
36 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Magnet stability
!
MQE = H (Tcs) "H (To)
(adiabatic)
!
MQE " cp To( ) Tc*(B) #To( ) 1#
I
Ic
$
% &
'
( ) 0,001
0,01
0,1
1
10
10 100
Cp (
MJ
/m3/K
)
Temperature (K)
Cu
He
Stability:magnet ability to tolerate an energy deposit (no quench)
Minimum Quench Energy (MQE)
# Low for LTS
# HeliumCooling improves LTS stability
37 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Magnet protection
Any SC magnet must be protected in case of a quench
Protection: temperature rise limitation(differential!contraction!stresses, material (resin) damages)
One of the most dangerous fault in a SMES: QUENCH
Protection:• Quench detection• Fast current reduction
+ adequate magnet design to prevent a quench andto limit its effect
38 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Basic magnet protection
Max. temperature reached after a quench(hot spot calculation)
!
F (Tmax ) = Jo2
Wmag
Vmax Io+ tdet ection
"
# $
%
& '
!
F (Tmax ) =cp (T )
" (T )To
Tmax
# dT
Power supply(current source)
SC coil(inductance L)
Protectionresistance
(Rd)
Tmax:
Vmax
Io
Quick detection
39 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
HTS magnet protection
Protection detectionis an issue!
vp "J
cp
#n $
T f %To
0,001
0,01
0,1
1
10
10 100
Cp (
MJ/m
3/K
)
Temperature (K)
Cu
He
HTS magnet protection is an issue!quench induces degradation
Tmax, dT/dz
SMES
Superconducting materials
41 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Superconducting materials
1G
2G
PIT BiSrCaCuOBi-2212 & Bi-2223
Coated conductorYBaCuO
10
100
1000
10000
100000
0 5 10 15 20 25 30
Jc (M
A/m
2)
Magnetic flux density (T)
20 K
20 K
50 K
50 K
77 K
77 K
Nb3Sn @ 4 K
NbTi @ 4 & 1,8 K
======= HTS =======
======= LTS =======
NbTi Nb3Sn
42 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES LTS conductor
Courtesy C. Luongo
• Cable in Conduct
• Developed & tested for
SMES ETM
• NbTi
• He @ 1.8 K
• Test: 200 kA, 5 T, 1.8 K
• Achieved 303 kA
(world record)
43 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Operating temperature
0
20
40
60
80
0 20 40 60 80 100
Cry
ogenic c
ost
(Carn
ot) (W
/W
)
Cold temperature Tf (K)
(Tc = 300 K)
20 K : 14 W/W
50 K : 5 W/W
4 K : 74 W/W
InterestHTS
&CC
10
100
1000
10000
0 2 4 6 8 10 12 14
Ic (A/cm)
Induction magnétique (T)
CC - 20 K
PIT - 20 K
PIT - 50 KCC - 50 K
CC - 77 KPIT - 77 K
" Cryogenic cost# running
# investment
" Stability# margins & perturbations
" Isolating thickness# voltage => power
0,0001
0,001
0,01
0,1
1
10
20 40 60 80 100
Cp (J/cm
3/K)
Temperature (K)
Cu
4 K : 1
20 K : 75
50 K : 900
=> Protection <=
SMES
HistoryExamples
45 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
History
! Introduced by Ferrier in 1969 to meet peak demands
! 30 MJ BPA experience
! 5-20 MWh / 100-500 MW ETM in the 80’ (SDI context)
! 3-6 MJ / 1 MW SMES in the 90’
– More secure sources for critical/sensitive loads (no voltage sags)
– FACTS
! First HTS «!large!» SMES in the 00’
46 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES evolutions
! LTS SMES– HTS current leads– Cryocoolers
– Power conditioning systems and control
! HTS SMES– Conductor developments (YBCO CC)
• Low cost• Mechanical properties• High current conductor
47 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
«!Commercial!» SMES
Trailerized Installation
GE Industrial Systems
Voltage Sag Protection
Power ratingsLoad voltage: 400 V to 20 kV
Unit Output: 1.3 MVA
Response Time: subcycle
System efficiency: > 97 %
Magnet (NbTi) dataStored energy: 3 MJ
Recharging time: < 90 s
Duty cycles nber: unlimited
SMES examples
48 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES SC (NbTi) magnet
SMES examples
49 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES as FACTS
! Voltage instability– voltage drop (50 %) )
D-SMES2,8 MVA2,0 MW
! 6 D-SMES– 90 % in less than 0.5 s
– 95 % in less than 1 s
– Grid capacity + 15 %
– Better voltage quality
SMES examples
50 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
CAPS 100 MJ SMES
Solenoid coil with pancakes
4 kA - 24 kV (96 MW)
86 MJ @ 4 kA
100 MJ @ 4.3 kA
CIC NbTi conductor
Courtesy C. Luongo
2 m
Stoped before completion
SMES examples
51 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Some HTS SMES
Grid stabilizationYBCOMJ class2012JapanChubu
Power qualityYBCO2.5 MJ2011KoreaKERI
Pulse appl.Bi-22120.8 MJ2007FranceDGACNRS
Power, voltagequality
Bi-22230.6 MJ2007KoreaKERI
Bi-22230.5 MVA, 1 MJ2007ChinaCAS
Voltage stabilityBi-22121 MVA, 1 MJ2004JapanChubu
ApplicationSCDataYearCountryOrgan.
52 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
800 kJ SMES project
• SMES potentialities for military uses– High power pulse sources (electric weapons)
Projects in progress
• Phase 1 (04-07) DGA - Nexans - CNRS
Basic technology of HTS SMES development
SMES HTS 800 kJ with “transparent” cryogenics
• Phase 2 (08-11) DGA - ISL - CNRS
HTS SMES suitable to electric gun development
Supply optimization
SMES performances (weigth)
53 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES HTS DGA/CNRS/ Nexans
Renforct
Kaptonisolation
3 solderedBi-2212tapes
• 800 kJ• Ø = 300 / 814 mm• h = 222 mm• I = 315 A• T = 20 K
Conductioncooling
Conductor based on Bi-2212 tapes
Projects in progress
54 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES HTS DGA/CNRS/ Nexans
-100
-50
0
50
100
0 50 100 150 200
Lower
Upper
Currents (A)
Time (s)
-100
-50
0
50
100
0 10 20 30 40
Lower
Upper
Currents (s)
Time (s)
Projects in progress
0
100
200
300
400
500
600
700
0 10 20 30 40 50 60 70 80
i1i2
i3iload
Curr
ents
(A)
Time (s)
55 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Korea (Keri)
• 2.5 MJ
• YBCO tapes (22 km)
• 550 A
• 20 K conduction cooled
• Bmax = 6.24 T
• Tests in 2011 ?
Power quality
56 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Japanese project
Courtesy of Chubu Electric
FACTSSystcontrol
Projects in progress
57 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
20 MJ LTS & HTS SMES
NbTi SMES with 4 K heliumpool boiling cooling system
YBCO SMES with 20 Kcryocooler cooling
Courtesy S. Nagaya
Projects in progress
58 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
New US SMES project (arpa)
Projects in progress
Partners: ABB, Brookhaven, SuperPower, Houston university
Specifications:• 2.5 MJ / 20 kW• Up to 25 T (4 K)• 2G wires
Objective:• Load levelling on thegrid with renewableenergies
SMES
Conclusions
60 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Conclusions
! Technology status– Currently available for short term power– Capability of SMES demonstrated– Successful experiences on years– Too high initial cost: the major bottleneck– Competition by more mature technologies
! Future– HTS, coated conductors
• Specific energy improvement• Reduced cryogenics
61 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
SMES : pulse current source
! SMES, best solution– In the intermediate range of power-energy plan or for
extreme powers
– for current type load
(batteries: energy sources, capacities: pulse voltage sources)
! Application examples– Electromagnetic launcher/catapult/gun
– Some FACTS, UPS (Uninterruptible Power Supply)
– Pulse applications (electron lasers, pulse field, ...)
Summary
62 P. TixadorInstitut Néel, G2Elab
2011 ESASSummer school
Some references
! W. Hassenzahl, “Superconducting Magnetic Energy Storage”, IEEETrans. On Magnetics, 1989, pp. 750-758.
! C. Luongo, “Superconducting Storage Systems: an overview”, IEEETrans. on Magnetics, Vol. 32, 1996, pp. 2214-2223.
! H. W. Lorenzen and al., “Small and fast-acting SMES”, Handbook ofApplied Superconductivity, B. Seeber, vol. 2, 1998 IOP, ISBN-10:0750303778.
! ASC, MT & EUCAS proceedings mainly