electromagnetic propulsion, suspension and levitation new ......electromagnetic propulsion,...
TRANSCRIPT
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• )
Electromagnetic Propulsion, Suspension and Levitation –
New Concepts of Bearingless Systems for High-Precision
Industry
Prof.dr. Elena Lomonova
Swiss Chapter of IEEE Power Electronics Society – 21.02.2020, ETH
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2Swiss Chapter of IEEE Power Electronics Society
Research areas • High-tech systems
– Linear and planar motors, magnetic
levitation
– Ultra-high precision power amplifiers
– Field modeling, materials, parasitic effects
– Wireless energy transfer
• Health– Power amplifiers for MRI and X-ray
– Medical robotics
– High-speed motors
• Sustainable energy– Smart grids
– Energy management, chargers, storage
– In-wheel motors and active suspension
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3Swiss Chapter of IEEE Power Electronics Society
Planar motors• Planar motor is an xy-positioning device
• Mover could be magnetically levitated
• First concept: Sawyer motor (1968)
– Stepper motor with air bearings
• Permanent magnet planar motors
– Semiconductor equipment
– Integrated magnetic bearings
(waferscanners)
– Air bearings (wafer dicing)
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4Swiss Chapter of IEEE Power Electronics Society
Planar motors• Planar motor is an xy-positioning device
• Mover could be magnetically levitated
• First concept: Sawyer motor (1968)
– Stepper motor with air bearings
• Permanent magnet planar motors
– Semiconductor equipment
– Integrated magnetic bearings
(waferscanners)
– Air bearings (wafer dicing)
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5Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
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6Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
light source
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7Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
lens
light source
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8Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
reticle
lens
light source
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9Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
reticle
lens
light source
lens
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10Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
reticle
wafer
lens
light source
lens
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11Swiss Chapter of IEEE Power Electronics Society
Application of planar stages
reticle
wafer
lens
light source
lens
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12Swiss Chapter of IEEE Power Electronics Society
Application of planar stagesSemiconductor lithography
planar
motor
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13Swiss Chapter of IEEE Power Electronics Society
Application of planar stagesSemiconductor lithography
• Process in the production of integrated
circuits (micro-processors)
wafer
short
stroke
long
stroke
planar
motor
integrated
circuit
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14Swiss Chapter of IEEE Power Electronics Society
Application of planar stagesSemiconductor lithography
lens
mask
light
source
• Process in the production of integrated
circuits (micro-processors)
• Accurate and fast positioning of the
wafer is crucial
Acceleration > 50 m/s2 (5 g)
Positioning accuracy < 1 nm
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15Swiss Chapter of IEEE Power Electronics Society
Application of planar stagesSemiconductor lithography
lens
mask
light
source
• Process in the production of integrated
circuits (micro-processors)
• Accurate and fast positioning of the
wafer is crucial
Acceleration > 50 m/s2 (5 g)
Positioning accuracy < 1 nm
• Typically dual-stage topology for 6-
DoF positioning of the wafer
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16Swiss Chapter of IEEE Power Electronics Society
Levitated and suspended planar stages
Contents
• Application
• Working principle
• Commutation
• Over-actuation
– Power minimization
– Heat distribution
– Force distribution
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17Swiss Chapter of IEEE Power Electronics Society
Moving coils –planar motor
courtesy of Philips
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18Swiss Chapter of IEEE Power Electronics Society
Moving-magnet planar motor
courtesy of TU/E
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19Swiss Chapter of IEEE Power Electronics Society
Moving-magnet planar motor
courtesy of TU/E
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20Swiss Chapter of IEEE Power Electronics Society
Magnetically levitated planar motor
• Production of force in x,y,z-directions
• Flux linkage variation in x,y,z-directions
A+ A- B+ B- C+ C-x
z
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21Swiss Chapter of IEEE Power Electronics Society
Magnetically levitated planar motor
• Production of force in x,y,z-directions
• Flux linkage variation in x,y,z-directions
• Instead of double sided actuator
A+ A- B+ B- C+ C-x
z
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22Swiss Chapter of IEEE Power Electronics Society
Magnetically levitated planar motor
• Production of force in x,y,z-directions
• Flux linkage variation in x,y,z-directions
• Single sided actuator
A+ A- B+ B- C+ C-x
z
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23Swiss Chapter of IEEE Power Electronics Society
Single-sided coreless motor (periodical section)
• Magnetic
flux φ
• Magnetic flux
density B
A+ A- B+ B- C+ C-
x
z
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24Swiss Chapter of IEEE Power Electronics Society
Single-sided coreless actuator
Levitation and propulsion force
can be decoupled
sin
4sin
3
8sin
3
a pm
b pm
c pm
z
z
z
x
x
ex
e
e
0
0
0
sin
4sin
3
8sin
3
a
b
c
xI I
xI I
xI I
0
, ,
0
, ,
3sin
2
3cos
2
z
nx n pm
n a b c
z
nz n pm
n a b c
F i Iex
F i Iez
A+ A- B+ B- C+ C-
x
z
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25Swiss Chapter of IEEE Power Electronics Society
Moving coil vs moving magnet
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26Swiss Chapter of IEEE Power Electronics Society
Moving-magnet vs moving-coil planar motor
• Magnet array is finite, increases modeling complexity
• Force is acting on coil volumes, torque arm is larger and
position dependent for moving-magnet planar motors
• Modeling and control is more complex in moving-magnet
case, however, the levitated structure is less complex
xz
xz
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27Swiss Chapter of IEEE Power Electronics Society
Halbach magnet array• Halbach magnet array
– Increased flux density near coils
– Intrinsic shielding of own fields
– Back-iron is unnecessary (magnetically no function)
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28Swiss Chapter of IEEE Power Electronics Society
Linear magnet array
Coil shape
• Rectangular
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29Swiss Chapter of IEEE Power Electronics Society
Planar Magnet array
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30Swiss Chapter of IEEE Power Electronics Society
Planar Magnet array
Coil shape
• Round
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31Swiss Chapter of IEEE Power Electronics Society
Planar Magnet array
Coil shape
• Rectangular
(45 degrees)
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32Swiss Chapter of IEEE Power Electronics Society
Planar Magnet array
Coil shape
• Rectangular
(45 degrees)
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33Swiss Chapter of IEEE Power Electronics Society
Round coils
• Flux density alternating in x,y,z
directions
• Round coils can be applied
which are limited in size
τ
x
y
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34Swiss Chapter of IEEE Power Electronics Society
Round coils
• Flux density alternating in x,y,z
directions
• Round coils can be applied
which are limited in size
τ
x
y
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35Swiss Chapter of IEEE Power Electronics Society
Round coils
• Flux density alternating in x,y,z
directions
• Round coils can be applied
which are limited in size
τ
x
y
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36Swiss Chapter of IEEE Power Electronics Society
Rectangular coils
• Long coils can be applied
• Forces in x and y directions
can be physically decoupled
x
y
τn
Fx=0
Fy=0
τn
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37Swiss Chapter of IEEE Power Electronics Society
Rectangular coils
• Long coils can be applied
• Forces in x and y directions
can be physically decoupled
x
y
τn
Coil length: 2nτn
τn
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38Swiss Chapter of IEEE Power Electronics Society
Decoupling/Commutation• Each coils produces a Lorentz force and torque due to
each magnet in the magnet array
22 2 sin 2 sin
40
4
4 cos
z z
n n
z
n
p p
y cx c
x z x z c y xy
n n
xy
y y z x c x z x
z
p
x c
z xy z x y c
n
p yp xF B i e T F y p B i e
BF T F p x F p F
B
p xF B i e T F p y
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39Swiss Chapter of IEEE Power Electronics Society
Decoupling/Commutation• Each coils produces a Lorentz force and torque due to each magnet
in the magnet array
• The interaction (forces and torque components) can be described on
the level of the
– Magnet array (rigid body approach)
– Individual magnets (force and torque distribution)
1, 2, ,
1, 2, ,
1, 2, ,
1, 2, ,
1, 2, ,
1, 2, ,
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
x x x n x
y y y n y
z z n zz
x x n xx
y y n yy
z z n zz
F F p F p F p
F F p F p F p
F p F p F pFw
T p T p T pT
T p T p T pT
T p T p T pT
1
2
..( )
..
..
n
i
i
p i
i
Γ
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40Swiss Chapter of IEEE Power Electronics Society
Decoupling/Commutation
• Commutation algorithm contains real-time model of all
interactions in the planar motor
• Model implemented in look-up tables
• Inverse is based on minimization of losses
• Outer-loop provides stability
Planar motor
Power amplifiers
Feedback/ Feedforward
controller
Commutation x
1( )i p w Γ
1
-
22, ( )min
pp i wP i R p w R
ΔΓΓ
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41Swiss Chapter of IEEE Power Electronics Society
Multi-physical model
Electromagnetic model
force and torque
Commutation
current
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42Swiss Chapter of IEEE Power Electronics Society
Multi-physical model
Electromagnetic model
force and torque
Commutation
current
Mechanical model
shape
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43Swiss Chapter of IEEE Power Electronics Society
Multi-physical model
Electromagnetic model
force and torque
Commutation
current
Mechanical model
shape
Thermal model
temperature
Over-actuation
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44Swiss Chapter of IEEE Power Electronics Society
Mechanical model1 3
2 4
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45Swiss Chapter of IEEE Power Electronics Society
Thermal model
Vertical Heat flux
OFF ON OFF
RzRzRz
Ry Ry
Ry Ry
RzRzRz
y
z
coil
cooling block
epoxy
Lateral Heat flux
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46Swiss Chapter of IEEE Power Electronics Society
Multi-physical framework
Electromagnetic modelforce and torque
Mechanical modelshape
Thermal modeltemperature
Commutationcurrent
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47Swiss Chapter of IEEE Power Electronics Society
Multi-physical framework
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48Swiss Chapter of IEEE Power Electronics Society
Electromagnetic model• Electromagnetic interactions between coils and magnets
x
z
y
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49Swiss Chapter of IEEE Power Electronics Society
Electromagnetic model• Electromagnetic interactions between coils and magnets
• Commutation defines currents from electromagnetic model
x
z
y
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50Swiss Chapter of IEEE Power Electronics Society
Electromagnetic model• Force and torque distribution on the magnet plate is
obtained from electromagnetic model
• Force and torque distribution, and currents are highly
position dependent
x
z
y
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51Swiss Chapter of IEEE Power Electronics Society
Mechanical model• Mechanical model coupled to electromagnetic model to
predict deformation
• Over-actuation allows reducing deformation
x
z
y
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52Swiss Chapter of IEEE Power Electronics Society
Thermal model• Temperature distribution is calculated from current
distribution
• Over-actuation allows reducing maximum temperature,
increasing maximum acceleration
x
z
y
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53Swiss Chapter of IEEE Power Electronics Society
Electromagnetic model• Electromagnetic interactions between coils and magnets
• Commutation defines currents from electromagnetic model
x
z
y
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54Swiss Chapter of IEEE Power Electronics Society
Electromagnetic model• Force and torque distribution on the magnet plate is
obtained from electromagnetic model
• Force and torque distribution, and currents are highly
position dependent
x
z
y
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55Swiss Chapter of IEEE Power Electronics Society
Mechanical model• Mechanical model coupled to electromagnetic model to
predict deformation
• Over-actuation allows reducing deformation
x
z
y
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56Swiss Chapter of IEEE Power Electronics Society
Mechanical model• Mechanical model coupled to electromagnetic model to
predict deformation
• Over-actuation allows reducing deformation
x
z
y
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57Swiss Chapter of IEEE Power Electronics Society
Mechanical model• Mechanical model coupled to electromagnetic model to
predict deformation
• Over-actuation allows reducing deformation
x
z
y
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58Swiss Chapter of IEEE Power Electronics Society
Mechanical model• Mechanical model coupled to electromagnetic model to
predict deformation
• Over-actuation allows reducing deformation
x
z
y
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59Swiss Chapter of IEEE Power Electronics Society
Thermal model• Temperature distribution is calculated from current
distribution
• Over-actuation allows reducing maximum temperature,
increasing maximum acceleration
x
z
y
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60Swiss Chapter of IEEE Power Electronics Society
Thermal model• Temperature distribution is calculated from current
distribution
• Over-actuation allows reducing maximum temperature,
increasing maximum acceleration
x
z
y
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61Swiss Chapter of IEEE Power Electronics Society
TopologiesSeveral moving-magnet planar motor topologies have been
manufactured and studied
HPPA (TU/e) EPM (Philips) COPAM (TU/e)
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62Swiss Chapter of IEEE Power Electronics Society
Comparison
Acceleration
Accuracy
Deformation
Goal: Combine advantages in a new design
x
x
x
x
topology
criterion
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63Swiss Chapter of IEEE Power Electronics Society
Double layer design
• Two layers of coils
• Height of the coils
optimized such that
dissipation per unit of
force is equal
• Phase shift in each layer
to reduce force ripples
Patent application filed
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64Swiss Chapter of IEEE Power Electronics Society
Power dissipation
Lowest mean
Dissipated power during full acceleration (50 m/s2):
Min [kW] Max [kW] Mean [kW]
HPPA 2.26 3.34 2.86
COPAM 3.22 4.44 3.80
EPM 3.33 4.12 3.65
DLPM 2.44 3.30 2.85
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65Swiss Chapter of IEEE Power Electronics Society
Trajectory - Temperature
Lowest temperature rise
Power dissipation [kW] Maximum temperature [oC]
HPPA 0.97 48
COPAM 1.4 57
EPM 1.2 59
DLPM 1.1 47
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66Swiss Chapter of IEEE Power Electronics Society
What limits the performance of a
single-stage planar motor?
cooling plates
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67Swiss Chapter of IEEE Power Electronics Society
What limits the performance of a
single-stage planar motor?
Eddy currents
• Induced in electrically conducting
materials
• Create a parasitic force
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68Swiss Chapter of IEEE Power Electronics Society
What limits the performance of a
single-stage planar motor?
Eddy currents
• Induced in electrically conducting
materials
• Create a parasitic force
Flexible behavior of the mover
• Excited by the force acting on the
permanent magnets
• Cause spatial deformation of the
mechanical structure
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69Swiss Chapter of IEEE Power Electronics Society
What limits the performance of a single-stage planar motor?
Eddy currents
• Induced in electrically
conducting materials
• Create a parasitic force
Flexible behavior of the mover
• Excited by the force acting on
the permanent magnets
• Cause spatial deformation of
the mechanical structure
cooling plates
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70Swiss Chapter of IEEE Power Electronics Society
Magnetically suspended, iron-core, planar motors
• Planar motor suspended from ceiling
• Moving-coils, stationary magnets
• Based on the same principles as a coreless levitated
planar motor
• Levitation without power consumption
Ceiling
Mover
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71Swiss Chapter of IEEE Power Electronics Society
Structure
• 4 iron-core linear motors
• 45 degrees rotated wrt
magnets
• Propulsion in x, and y
• Passive attraction force
Bottom view Side view
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72Swiss Chapter of IEEE Power Electronics Society
Principles
• Controlled as three-phase motor
• Small force ripples
• Only considerable torque Ty
Laminated iron yoke
Permanent magnets
Coils
Nonferromagnetic plate
Fx
FzZero current
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73Swiss Chapter of IEEE Power Electronics Society
Principles
• Controlled as three-phase motor
• Small force ripples
• Only considerable torque Ty
Laminated iron yoke
Permanent magnets
Coils
Nonferromagnetic plate
Fx
Fzd-axis current
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74Swiss Chapter of IEEE Power Electronics Society
Principles
• Controlled as three-phase motor
• Small force ripples
• Only considerable torque Ty
Laminated iron yoke
Permanent magnets
Coils
Nonferromagnetic plate
Fx
Fzq-axis current
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75Swiss Chapter of IEEE Power Electronics Society
Magnetic loading
• Fz,r is proportional to magnetic flux density B
• Motor constant k is proportional to B
• Magnet with low remanence, limited acceleration
k >
Magnetic suspension Acceleration Torque compensation
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76Swiss Chapter of IEEE Power Electronics Society
Contactless power supply
• Power supply through resonant inductive coupling with
low position variation
• Plastic bonded magnets required (with low remanence Br)
to reduce eddy current losses
Switched
primary coil array
(yellow coils active)
Secondary coil
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77Swiss Chapter of IEEE Power Electronics Society
Realization• planar stroke: 200x200 mm2
• nominal acceleration: 5 ms-2
• power transfer: 335 W
• variation power transfer: 15%
• Mover size: 37x37 cm2
• moving mass: 9 kg
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78Swiss Chapter of IEEE Power Electronics Society
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79Swiss Chapter of IEEE Power Electronics Society
Conclusions• Planar stages could be levitated or suspended
• 45 degrees rotated coil cannot only be used in coreless,
but also iron-core planar motors
• Balance between acceleration, suspension force and
mass in multi-physical design
• Integration of energy transfer system in the airgap
requires magnets with a low electric conductivity (and
hence, with a low magnetic loading)
• Superconducting motors are the next generation of planar
stages
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80Swiss Chapter of IEEE Power Electronics Society
Thank you for your attention
Acknowledgements:
dr. J. Jansen, dr. T. Overboom, dr. J. Smeets,
dr. J. de Boeij, dr. H. Rovers, dr. C. Custers
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• )
Electromagnetic Propulsion, Suspension and Levitation –
New Concepts of Bearingless Systems for High-Precision
Industry
Prof.dr. Elena Lomonova
Swiss Chapter of IEEE Power Electronics Society – 21.02.2020, ETH