160610 esas reis ho - unibo.it · t. reis, j. oswald, b. oswald, a.t.a.m. dewaele oswald...

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TR 2016 ESAS International Summer School 1 T. Reis, J. Oswald, B. Oswald, A.T.A.M. deWaele Oswald Elektromotoren GmbH www.oswald.de superconducting rotating machines

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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

TR 2016 ESAS International Summer School 4

Oswald Elektromotoren GmbH

TR 2016 ESAS International Summer School 5

Oswald Elektromotoren GmbH

50 kW … 2 MW customized motors/generators … 200.000 Nm

TR 2016 ESAS International Summer School 6

motor / generator

FJ

B

J

F

functional principle of a homopolar motor

resulting lorentz force on current in external field

TR 2016 ESAS International Summer School 7

motor / generator

http://www.fh-sw.de/sw/fachb/et/labinfo/em/iSEE/dreh.htm

TR 2016 ESAS International Summer School 8

motor / generator

spacial arrangement of coils number of slotsnumber of polesnumber of phasesconnectionpowerspeed

TR 2016 ESAS International Summer School 9

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 12

motor / generator

RPHI

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

TR 2016 ESAS International Summer School 15

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

TR 2016 ESAS International Summer School 16

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

TR 2016 ESAS International Summer School 17

motor / generator

TR 2016 ESAS International Summer School 18

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

TR 2016 ESAS International Summer School 19

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

TR 2016 ESAS International Summer School 21

motor / generator

Advantages of PM-Motors:

- High force density

- Passive rotor

- High dynamics

… enables many

new applications

4 poles 16 poles

TR 2016 ESAS International Summer School 22

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 23

motor / generator

Quelle: Vestas

no nc solutionsso far…

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 25

motor / generator

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

TR 2016 ESAS International Summer School 27

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

?

TR 2016 ESAS International Summer School 30

motor / generator

�: ������turns�: �����

����������������

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 35

motor / generator

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

TR 2016 ESAS International Summer School 39

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

TR 2016 ESAS International Summer School 40

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 70

SC losses in AC application

RPHI

B

B

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 80

SC losses in AC application

Quelle: CryoZone

fan

TR 2016 ESAS International Summer School 81

SC losses in AC application

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 83

SC losses in AC application

TR 2016 ESAS International Summer School 84

operation temperaturedepends on load:

lossescooling capacity

cooling system of SC in stator

TR 2016 ESAS International Summer School 85

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

TR 2016 ESAS International Summer School 87

potential of SC-motors:

- power density> 200%- dynamics > 300%- weight/size 40…60%- efficiency …99,7%- availability of material

applications:

- mobility (ship, vehicle, plane)- generators- industrial drives

SC – motors:Oswald