160610 esas reis ho - unibo.it · t. reis, j. oswald, b. oswald, a.t.a.m. dewaele oswald...
TRANSCRIPT
TR 2016 ESAS International Summer School 1
T. Reis, J. Oswald, B. Oswald, A.T.A.M. deWaeleOswald Elektromotoren GmbH
www.oswald.de
superconducting
rotating machines
TR 2016 ESAS International Summer School 2
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 3
Karl Oswald und Sohn
foundation 1909 in Miltenberg am Main
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Oswald Elektromotoren GmbH
50 kW … 2 MW customized motors/generators … 200.000 Nm
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motor / generator
FJ
B
J
F
functional principle of a homopolar motor
resulting lorentz force on current in external field
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motor / generator
http://www.fh-sw.de/sw/fachb/et/labinfo/em/iSEE/dreh.htm
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motor / generator
spacial arrangement of coils number of slotsnumber of polesnumber of phasesconnectionpowerspeed
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motor / generator
3 m
60.000 Nm 2 tons
350 Nm
P~M⋅f/p P: Powerf: Frequencyp: number of pole pairs
TR 2016 ESAS International Summer School 10
motor / generator
P~M⋅f/p
n [rpm]
Is
M
P
U
Up
Umax
rated operation
TR 2016 ESAS International Summer School 11
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 13
motor / generator
external field
flux in material
in air
TR 2016 ESAS International Summer School 14
motor / generator
NdFeB:B = 1,1 - 1,3T
iron:Bmax = 2T
magnetically softmagnetically hard
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motor / generator
NdFeB:B = 1,1 - 1,3T
iron:Bmax = 2T
80% coverage 50% coverage
Flux densityin Airgap:B = 1T
PM-Synchonous motor:All parts fit perfect together
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motor / generator
0
10
20
30
40
50
60
70
80
90
100
1980 1984 1988 1992 1996 2000 2004 2008 2012 2016
%
DC
AC asynchron
AC synchron
DC motorsuntil 80‘s
development of inverter technology:efficient asynchronous motors
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motor / generator
0
10
20
30
40
50
60
70
80
90
100
1980 1984 1988 1992 1996 2000 2004 2008 2012 2016
%
DC
AC asynchron
AC synchron
PM-synchronous motors
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motor / generator
development of NdFeB-Magnets decisivefor synchronous technology:
- increased force density (>20%)- higher efficiency (some %)- more compact (> 1 size)- better dynamics (>30%)- …
TR 2016 ESAS International Summer School 20
motor / generator
Que
lle: S
chul
er/B
MW
power: 390 kW
torque: 15500 Nm
weight: 2310 kg
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motor / generator
Advantages of PM-Motors:
- High force density
- Passive rotor
- High dynamics
… enables many
new applications
4 poles 16 poles
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motor / generator
0
10
20
30
40
50
60
70
80
90
100
1980 1984 1988 1992 1996 2000 2004 2008 2012 2016
%
DC
AC asynchron
AC synchron
next developments?
What is needed?
TR 2016 ESAS International Summer School 24
motor / generator
- solutions for so farunfulfillable requests
- independance oncritical resources
- new applicationspossible
- usage of newtechnologies andmaterials for buildingmotors
- improvement ofoperating parameters
- …
TR 2016 ESAS International Summer School 26
motor / generator
superconducting
transmission linessuperconducting
propulsion motors
superconducting
generator + turbine
power electronics
batteries
EADS/Airbus concept: Paris Air show 2013
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New applications are arising:
- Increased acceleration rate
- Reduced Size
- Increased power density
Common background:
even applications are in development
years to come into market…
motor / generator
TR 2016 ESAS International Summer School 28
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 29
motor / generator
el. power
iron losses
copper losses
copper losses
stator
rotor
friction, iron losses
mech. power
?
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motor / generator
�: ������turns�: �����
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limiting factors:- available space for magnetic system- space needed for application- cooling system
�~��
engineering current density: �~��
� �
TR 2016 ESAS International Summer School 31
motor / generator
Bilder von Spulen!j / A/mm² B / T cooling
2 - 4 0,05 conduction
5 - 10 0,1 water jacket
Quelle: Superpower
TR 2016 ESAS International Summer School 32
motor / generator
j / A/mm² B / T cooling
2 - 4 0,05 conduction
5 - 10 0,1 water jacket
20 - 40 1 hollow conductor
Quelle: Superpower
TR 2016 ESAS International Summer School 33
motor / generator
j / A/mm² B / T cooling
2 - 4 0,05 conduction
5 - 10 0,1 water jacket
20 - 40 1 hollow conductor
> 150 > 10 superconductor
Quelle: Superpower
TR 2016 ESAS International Summer School 34
motor / generator
current density:
superconducting layer> 60.000 A/mm²
tape> 600 A/mm²
engineering> 150 A/mm²
j / A/mm² B / T cooling
2 - 4 0,05 conduction
5 - 10 0,1 water jacket
20 - 40 1 hollow conductor
> 150 > 10 superconductor
Quelle: Superpower
TR 2016 ESAS International Summer School 36
motor / generator
Quelle: Izumi, Japan
trade off:
- critical current
- operating
temperature
- availability
- price
- dimensions
- losses
- …
TR 2016 ESAS International Summer School 37
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 38
motor topologies
AC – nc asynchronous rotor
nc – PM-Rotor – sc
nc – rotor sep. excited– sc
nc – reluctance rotor – sc
all sc motor
… and some more:
homopolar
axial flux
transversal flux
…reference motor
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reluctance motor
- Diamagnetic rotor
- Passive rotor – no power transmission
- Cold rotor
- Iron in rotor obligational and close to SC
- Relative low force density
- No limitations in operation
- Complex rotor structure – speed limitations
Force density:
130% compared to nc PM-Motor
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excited Synchronous Motor
- Active SC coils in rotor (DC application)
- power transmission (many kA!)
- Cold rotor
- Iron in rotor (partially) useless (>2T?)
- Active influence on excitation
- Complex rotor structure – speed limitations
and minimum sizing (-> MW)
Force density:
> 200% compared to nc PM-Motor
TR 2016 ESAS International Summer School 41
PM motor
- Active SC coils in stator (AC application)
- Passive rotor system
- Cold stator
- Iron in stator (partially) useless (>2T?)
- Flux control for high speed
- Cryostat for rotating fields
Force density:
> 250% compared to nc PM-Motor
TR 2016 ESAS International Summer School 42
fully SC motor (exc. rotor)
- Active SC coils in stator (AC application)
- Active SC coils in rotor (DC application)
- Cold stator and rotor
- Iron in stator and rotor (partially) useless
- Power transmission to rotor (many kA!)
- Active influence on excitation
- Complex rotor structure – speed limitations
and minimum sizing (-> MW)
Force density:
> 300% compared to nc PM-Motor
TR 2016 ESAS International Summer School 43
fully SC motor (bulk rotor)
- Active SC coils in stator (AC application)
- Bulk SC in rotor (DC application)
- Cold stator and rotor
- Iron in stator and rotor (partially) useless
- Passive rotor
- Magnetizing device needed
- Flux control for high speed or dynamic
adaption of magnetization
Force density:
> 300% compared to nc PM-Motor
TR 2016 ESAS International Summer School 44
Homopolar motor
- Active SC coils in stator (DC application)
- Rotor made of conductive material
- Cold stator
- Iron in stator and rotor (partially) useless
- Power transmission (many kA!)
at least one at large diameter !!!
- Easy speed control
Force density:
> 200% compared to nc PM-Motor
TR 2016 ESAS International Summer School 45
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 46
SC motors / generators
power / MVA speed / rpm application
Converteam UK 1,79 214 hydro generator
Siemens Germany 4 120 ship propulsion motor
Converteam UK 8 12 wind generator
AMSC USA 36,5 120 ship propulsion motor
Siemens Germany 4 3600 industrial generator
Converteam UK 0,5 nn demo generator
IHI marine Japan 0,365 200 ship propulsion motor
Doosan, KERI Korea 1 3600 demo motor
Doosan, KERI Korea 1 1800 demo generator
Kawasaki Japan 1 190 ship propulsion motor
AMSC USA 8 1800 generator
AMSC USA 5 230 motor
Oswald Germany 0,2 650 industrial motor
TR 2016 ESAS International Summer School 47
SC specific features:
- „R=0“, only inductance ofexcitation coil
- feeding of high rotorcurrents
- flux guidance in yoke andteeth (saturation!)
- mech. power transmission
- …
increase of „B“ by SC-excitation coils in the rotor
motor topologies
TR 2016 ESAS International Summer School 48
magn. air gap
cooling
HTS-coilcryostat
pole core
SC specific features:
- thermal insulation of rotor
- feeding of coolant
- temperature drop > 200K
Quelle: Siemens
advantage: DC-application
no losses in SC
motor topologies
increase of „B“ by SC-excitation coils in rotor
TR 2016 ESAS International Summer School 49
Quelle: GE
SC – motors:GE
1970’s - Westinghouse5 MW, 4.5 K NbTi Superconductor
1980’s -General Electric20 MW, 4.5/8 KNbTi/Nb3Sn Superconductor
1990’s – Westinghouse STC1 MW, 20 KBSCCO Superconductor
TR 2016 ESAS International Summer School 50
Quelle: Siemens Quelle: Siemens
Quelle: Siemens
HTS II:
2002 - 20074 MVA3600 rpm
high speedlongterm operationsince 2009
HTS I:
1999 - 2002400 kW1500 rpm
technologydemonstrator
HTS III:
2006 - 20104 MW120 rpmhigh torque: 300 kNm
SC – motors:Siemens
TR 2016 ESAS International Summer School 51
Quelle: Siemens
HTS I:
1999 - 2002400 kW1500 rpm
technologydemonstrator
SC – motors:Siemens
Synchronous motorBi2223/AG tapeAir gap copper stator
Operating temperature 27K„plug and play“
Ne cooling system
TR 2016 ESAS International Summer School 52
Quelle: Siemens
HTS I:
1999 - 2002400 kW1500 rpm
technologydemonstrator
SC – motors:Siemens
TR 2016 ESAS International Summer School 53
Quelle: Siemens
HTS I:
1999 - 2002400 kW1500 rpm
technologydemonstrator
SC – motors:Siemens
TR 2016 ESAS International Summer School 54
Quelle: Siemens
HTS II:
2002 - 20074 MVA3600 rpm
high speedlongterm operationsince 2009
SC – motors:Siemens
TR 2016 ESAS International Summer School 55
first operation in test rig
Quelle: Siemens
Quelle: Siemens
Siemens 4MW HTS II 2007 at test rig:
- rotor at 25K (fl. Ne)
- motor weight -30%
- coils made of Bi-2223
- first grid synchronization 2009
- efficiency +2%
- losses -50%
- > 5000 hours of operation withoutdegradation of SC
TR 2016 ESAS International Summer School 56
GE Hydrogenie:
2006 - 20131,7 MW
214 rpm
HTS-coils on rotor
cooling with He-gas-feedthrough in shaft
Quelle: GE
SC – motors:GE
TR 2016 ESAS International Summer School 57
AMSC ship propulsion:
36,5 MW120 rpm
Quelle: AMSCQuelle: AMSC
SC – motors:AMSC
TR 2016 ESAS International Summer School 58
SC – motors:Oswald
SDYN110:
400 kW77 K, lN 2
reluctance type motorpower density 130% compared to nc PM-motor
TR 2016 ESAS International Summer School 59
SC – motors:Oswald
Plastic:Po = 229 kWPa= 470 kVA
Ideal SC:Po = 345 kWPa= 400 kVA
Real YBCO:Po = 256 kWPa= 420 kVA
TR 2016 ESAS International Summer School 60
SC – motors:wind power
Quelle: tecnalia
Superturbine:10MW offshore by 2020
ecoswing:3MW onshore retrofit
TR 2016 ESAS International Summer School 61
Quelle: AMSCQuelle: Siemens
Quelle: eco5
10MW sc 4MW pm8MW ind
advantage SC motors:
volume-40…60%
weight-50…70%
power density+100…150%
dynamics+150…200%
efficiency…99,9%
SC – motors:DC-application in rotor
TR 2016 ESAS International Summer School 62
motor / generator
SC specific features:
- cooling in the not movingparts
- AC-application of SC:
many constraints!
increase of „A“ by SC-field coils in the stator
TR 2016 ESAS International Summer School 63
SC – motors:Oswald
SLIN:
45 kN77 K, lN 2
stator coils BSCCOpower density andacceleration: 200%
TR 2016 ESAS International Summer School 64
SC – motors:Oswald
SMFS:
40 kW, 665 rpm, 575 Nm77 K, lN 2
PM-motor with SC statorpower density 200%compared to nc PM-motor
TR 2016 ESAS International Summer School 65
Why can SC be useful in a motor/generator
how do motors work
what are todays limitations for motors
where can SC be used in a motor
topologies and examples
cryogenic aspects
outline
TR 2016 ESAS International Summer School 66
SC losses in AC application
low temperature – SC:
in mixed phase flux lines through SCwith each elementary flux quantum:h/2e = 2,07 10-15 Tm²
TR 2016 ESAS International Summer School 67
- transport current causes Lorentz force on flux lines
- drifting movement consumes energy, appearing as el. resistance
- defects in cristal lattice can pin fluxlines
- flux lines are pinned until criticalcurrent density, resistance disappears
SC losses in AC application
TR 2016 ESAS International Summer School 68
B
I
B
B?
SL: 5x 1µmStack: 1,3mm
I I?
losses in single tapecan be calculated analytically
good analytical approximationfor ideal stack
behavior in coil shape, with ext. fields, alternating current, shielding, …?
SC losses in AC application
TR 2016 ESAS International Summer School 69
influence oncrit. current
SC losses in AC application
Losses in single tape in selffield can be calculated
Approximation for stack (part of coil in slot):
- Losses due to current transport in selffield:
- Losses due to external magnetic field:
TR 2016 ESAS International Summer School 71
SC losses in AC application
BB
Calculation of magn. Flux within SC
TR 2016 ESAS International Summer School 72
with material data and boundary conditions (ext. field, current, temperature, …):losses in SC can be estimated.
SC losses in AC application
TR 2016 ESAS International Summer School 73
with material data and boundary conditions (ext. field, current, temperature, …):losses in SC can be estimated.
Lo
ss i
n S
C a
nd
iro
n[%
of lo
ss a
t rat
ed v
alu
es]
Torque [kNm]
262218
20
40
60
80
100
0 141062
AC total
V Fe
P trans
P hyst
SC losses in AC application
TR 2016 ESAS International Summer School 74
calorimetric measurementof SC losses:
- ext. magn. field
- current transport
- self field
- temperaturedependence
SC losses in AC application
TR 2016 ESAS International Summer School 75
SC losses in AC application
losses with current transport in Racetrack-coils in selffield:measurement (kalorimetric und elektrical) vs. calculation
Additional losses(quench)
TR 2016 ESAS International Summer School 76
SC losses in AC application
Cooling technology:
• Direct contact / heat conduction
• Cooling with Gas, Liquid, …
heat capacity, evaporation energy, …
closed, open loop, …
TR 2016 ESAS International Summer School 77
Cooling technology:
• Direct contact / heat conduction
• Cooling with Gas, Liquid, …
heat capacity, evaporation energy, …
closed, open loop, …
SC losses in AC application
TR 2016 ESAS International Summer School 78
cooling system of SC in stator
optimal operation pointdepends on:
- SC material properties
- recooling of losses
- specifications
- size
- …
TR 2016 ESAS International Summer School 79
Quelle: Sumitomo
cooler:input power/cooling power
cooling system of SC in stator
cryocooler
TR 2016 ESAS International Summer School 82
SC losses in AC application
1. Ventilating system
2. Cold head
3. Power terminal (warm)
4. Transfer lines to motor
5. Sensoric terminal (cold)
6. Power terminal (cold)
7. Power transmission (cold-warm)
8. Heat exchanger
TR 2016 ESAS International Summer School 84
operation temperaturedepends on load:
lossescooling capacity
cooling system of SC in stator
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SC – motors:Oswald
Our goal:Turn white fog into black box
TR 2016 ESAS International Summer School 86
power:speed:torque:efficiency:dynamics:YBCOcc-tape:
40665575
99,6>10.000
400
kWrpmNm%rpm/sm
SC – motors:Oswald