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MESIN LISTRIK
Pertemuan 11
2Sean DeHart
3
4
5
6
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8
Electric Motor Basic Principles
 Interaction between magnetic field and current
carrying wire produces a force
 Opposite of a generator
Sean DeHart
9
Conventional (Brushed) DC Motors
 Permanent magnets
for outer stator
 Rotating coils for inner
rotor
 Commutation
performed with metal
contact brushes and
contacts designed to
reverse the polarity of
the rotor as it reaches
horizontal
Sean DeHart
10
2 pole brushed DC motor commutation
Sean DeHart
11
Conventional (Brushed) DC Motors
 Common Applications:
Small/cheap devices such as toys, electric tooth
brushes, small drills
Lab 3
 Pros:
Cheap, simple
Easy to control - speed is governed by the voltage and
torque by the current through the armature
 Cons:
Mechanical brushes - electrical noise, arcing, sparking,
friction, wear, inefficient, shorting
Sean DeHart
12
DC Motor considerations
 Back EMF - every motor is also a generator
 More current = more torque; more voltage = more speed
 Load, torque, speed characteristics
 Shunt-wound, series-wound (aka universal motor),
compound DC motors
Sean DeHart
13
Brushless DC Motors
 Essential difference - commutation is performed
electronically with controller rather than
mechanically with brushes
Sean DeHart
14
Brushless DC Motor Commutation
 Commutation is performed electronically using a
controller (e.g. HCS12 or logic circuit)
Similarity with stepper motor, but with less #
poles
Needs rotor positional closed loop feedback: hall
effect sensors, back EMF, photo transistors
Sean DeHart
15
Delta               Wye
BLDC (3-Pole) Motor Connections
 Has 3 leads instead of 2 like brushed DC
 Delta (greater speed) and Wye (greater torque)
stator windings
Sean DeHart
16
Brushless DC Motors
 Applications
CPU cooling fans
CD/DVD Players
Electric automobiles
 Pros (compared to brushed DC)
Higher efficiency
Longer lifespan, low maintenance
Clean, fast, no sparking/issues with brushed contacts
 Cons
Higher cost
More complex circuitry and requires a controller
Sean DeHart
AC Motors
Two main types of AC motor, Synchronous and
Induction.
Synchronous motors supply power to both the rotor
and the stator, where induction motors only supply
power to the stator coils, and rely on induction to
generate torque.
17Sean DeHart
18
AC Induction Motors (3 Phase)
 Use poly-phase (usually 3) AC current to create a rotating
magnetic field on the stator
 This induces a magnetic field on the rotor, which tries to
follow stator - slipping required to produce torque
 Workhorses of the industry - high powered applications
Sean DeHart
AC induction Motors
Induction motors only supply current to the stator,
and rely on a second induced current in the rotor
coils.
This requires a relative speed between the rotating
magnetic field and the rotor. If the rotor somehow
matches or exceeds the magnetic field speed, there is
condition called slip.
Slip is required to produce torque, if there is no slip,
there is no difference between the induced pole and
the powered pole, and therefore no torque on the
shaft.
19Sean DeHart
Synchronous AC Motors
Current is applied to both the Rotor and the Stator.
This allows for precise control (stepper motors), but
requires mechanical brushes or slip rings to supply
DC current to the rotor.
There is no slip since the rotor does not rely on
induction to produce torque.
20Sean DeHart
Stepper Motor
A stepper motor is an electromechanical device which
converts electrical pulses into discrete mechanical
movements. The shaft or spindle of a stepper motor
rotates in discrete step increments when electrical
command pulses are applied to it in the proper sequence.
Smriti Chopra
Main features
The sequence of the applied pulses is directly related to the
direction of motor shafts rotation.
The speed of the motor shafts rotation is directly related
to the frequency of the input pulses.
The length of rotation is directly related to the number of
input pulses applied.
Smriti Chopra
Stepper Motor Characteristics
  Open loop
The motors response to digital input pulses provides open-loop
control, making the motor simpler and less costly to control.
   
Brushless
   Very reliable since there are no contact brushes in the motor.
Therefore the life of the motor is simply dependant on the life of
the bearing.
Incremental steps/changes
The rotation angle of the motor is proportional to the input
pulse.
Speed increases -> torque decreases
Smriti Chopra
Torque vs. Speed
Torque varies inversely with
speed.
Current is proportional to
torque.
Torque ∞ means Current ∞,→ →
which leads to motor damage.
Torque thus needs to be limited
to rated value of motor.
Smriti Chopra
Disadvantages of stepper motors
There are two main disadvantages of stepper motors:
Resonance can occur if not properly controlled.
This can be seen as a sudden loss or drop in torque at certain speeds which can
result in missed steps or loss of synchronism. It occurs when the input step pulse rate
coincides with the natural oscillation frequency of the rotor. Resonance can be
minimised by using half stepping or microstepping.
Not easy to operate at extremely high speeds.
25
Working principle
Stepper motors consist of a permanent magnet rotating
shaft, called the rotor, and electromagnets on the
stationary portion that surrounds the motor, called the
stator.
When a phase winding of a stepper
motor is energized with current, a
magnetic flux is developed in the
stator. The direction of this flux is
determined by the “Right Hand
Rule”.
Smriti Chopra
At position 1, the rotor is
beginning at the upper
electromagnet, which is
currently active (has voltage
applied to it).
To move the rotor clockwise
(CW), the upper
electromagnet is deactivated
and the right electromagnet is
activated, causing the rotor to
move 90 degrees CW, aligning
itself with the active magnet.
This process is repeated in the
same manner at the south and
west electromagnets until we
once again reach the starting
position.
Smriti Chopra
Understanding resolution
Resolution is the number of degrees rotated per step.
Step angle = 360/(NPh * Ph) = 360/N
NPh = Number of equivalent poles per phase = number of rotor
poles.
Ph = Number of phases.
N = Total number of poles for all phases together.
Example: for a three winding motor with a rotor having 4 teeth,
the resolution is 30 degrees.
Smriti Chopra
Two phase stepper motors
There are two basic winding arrangements for the
electromagnetic coils in a two phase stepper motor:
bipolar and unipolar.
unipolar bipolar
Smriti Chopra
A unipolar stepper motor has two windings per phase, one
for each direction of magnetic field. In this arrangement a
magnetic pole can be reversed without switching the
direction of current.
Bipolar motors have a single winding per phase. The
current in a winding needs to be reversed in order to
reverse a magnetic pole.
Bipolar motors have higher torque but need more complex
driver circuits.
Main difference
Smriti Chopra
Stepping modes
Wave Drive (1 phase on)
A1 – B2 – A2 – B1
(25% of unipolar windings , 50% of bipolar)
Full Step Drive (2 phases on)
A1B2 – B2A2 – A2B1 – B1A1
(50% of unipolar windings , full bipolar
windings utilization)
Half Step Drive (1 & 2 phases on)
A1B2 – B2 – B2A2 – A2 ----
(increases resolution)
Microstepping (Continuously
varying motor currents)
A microstep driver may split a full step into as many as 256 microsteps.
Smriti Chopra
Types of Stepper Motors
There are three main types of stepper motors:
Variable Reluctance stepper motor
Permanent Magnet stepper motor
Hybrid Synchronous stepper motor
Smriti Chopra
This type of motor consists of a soft iron multi-toothed
rotor and a wound stator.
When the stator windings are energized
with DC Current, the poles become magnetized.
Rotation occurs when the rotor teeth
are attracted to the energized stator
poles.
Variable Reluctance motor
Smriti Chopra
Permanent Magnet motor
The rotor no longer has teeth as with
the VR motor.
Instead the rotor is
magnetized with alternating north
and south poles situated in a straight
line parallel to the rotor shaft.
These magnetized rotor poles provide an increased
magnetic flux intensity and because of this
the PM motor exhibits improved torque characteristics
when compared with the VR type.
Smriti Chopra
Hybrid Synchronous motor
The rotor is multi-toothed like the VR motor and
contains an axially magnetized concentric
magnet around its shaft.
The teeth on the rotor provide an even
better path which helps guide the
magnetic flux to preferred locations in
the air gap.
Smriti Chopra
Applications
Stepper motors can be a good choice whenever controlled
movement is required.
They can be used to advantage in applications where you
need to control rotation angle, speed, position and
synchronism.
These include
 printers
 plotters
 medical equipment
 fax machines
 automotive and scientific equipment etc.
Smriti Chopra
Linear Motors
Hannes Daepp
Hannes Daepp
Basics of Linear Motors [1],[4]
I
Analogous to Unrolled DC Motor
• Force (F) is generated
when the current (I)
(along vector L) and the
flux density (B) interact
• F = LI x B
Hannes Daepp
Linear Motors in Action
 http://www.parkermotion.com/video/Braas_Trilogy_T3E_Video.MPG
Hannes Daepp
Analysis of Linear Motors [1],[5]
Analysis is similar to that of rotary machines
Linear dimension and displacements replace
angular ones
Forces replace torques
Commutation cycle is distance between two
consecutive pole pairs instead of 360 degrees
Hannes Daepp
Benefits of Linear Motors [2]
High Maximum Speed
Limited primarily by bus voltage, control electronics
High Precision
Accuracy, resolution, repeatability limited by feedback device, budget
Zero backlash: No mechanical transmission components.
Fast Response
Response rate can be over 100 times that of a mechanical
transmission  faster accelerations, settling time (more throughput)
Stiffness
No mechanical linkage, stiffness depends mostly on gain & current
Durable
Modern linear motors have few/no contacting parts  no wear
Hannes Daepp
Downsides of Linear Motors [2]
Cost
Low production volume (relative to demand)
High price of magnets
Linear encoders (feedback) are much more expensive than rotary
encoders, cost increases with length
Higher Bandwidth Drives and Controls
Lower force per package size
Heating issues
Forcer is usually attached to load  I2
R losses are directly coupled to
load
No (minimal) Friction
No automatic brake
Hannes Daepp
Components of Linear Motors
[2],[3]
Forcer (Motor Coil)
Windings (coils) provide current (I)
Windings are encapsulated within core
material
Mounting Plate on top
Usually contains sensors (hall effect
and thermal)
Magnet Rail
Iron Plate / Base Plate
Rare Earth Magnets of alternating
polarity provide flux (B)
Single or double rail
F =
lI x B
Hannes Daepp
Types of Linear Motors [1],[2],[3]
Iron Core
 Coils wound around
teeth of laminations
on forcer
Ironless Core
 Dual back iron
separated by spacer
 Coils held together
with epoxy
Slotless
 Coil and back iron
held together with
epoxy
Hannes Daepp
Linear Motor Types: Iron Core [1],[2]
Distinguishing Feature
 Copper windings around forcer laminations over a single magnet rail
Advantages:
 Highest force available per unit volume
 Efficient Cooling
 Lower cost
Disadvantages:
 High attractive force between forcer & magnet track
 Cogging: iron forcer affects thrust
force as it passes over each
magnet (aka velocity ripple)
Hannes Daepp
Distinguishing Feature
 Forcer constructed of wound coils held
together with epoxy and running
between two rails (North and South)
 Also known as “Aircore” or “U-channel”
motors
Advantages:
 No attractive forces in forcer
 No Cogging
 Low weight forcer - No iron means
higher accel/decel rates
Top View
Forcer
Mounting
Plate
Rare
Earth
Magnets
Horseshoe
Shaped
backiron
Winding, held
by epoxy
Hall Effect and
Thermal
Sensors in coil
Front View
Linear Motor Types: Ironless [1],[2]
Disadvantages:
 Low force per package size
 Lower Stiffness; limited max load without improved structure
 Poor heat dissipation
 Higher cost (2x Magnets!)
Hannes Daepp
Distinguishing Feature
 Mix of ironless and iron core: coils with
back iron contained within aluminum
housing over a single magnet rail
Advantages over ironless:
 Lower cost (1x magnets)
 Better heat dissipation
 Structurally stronger forcer
 More force per package size
Advantages over iron core:
 Lighter weight and lower inertia forcer
 Lower attractive forces
 Less cogging
Side View
Front View
Back
iron
Mounting
plate
Coil
assemblyThermal
sensor
Rare
Earth
Magnets
Iron
plate
Linear Motor Types: Slotless [1],[2]
Hannes Daepp
Disadvantages
 Some attractive force and cogging
 Less efficient than iron core and
ironless - more heat to do the same job
Side View
Front View
Back
iron
Mounting
plate
Coil
assemblyThermal
sensor
Rare
Earth
Magnets
Iron
plate
Linear Motor Types: Slotless [2],[3]
Hannes Daepp
Linear Brushless DC Motor Type
Feature Iron Core Ironless Slotless
Attraction Force Most None Moderate
Cost Medium High Lowest
Force Cogging Highest None Medium
Power Density Highest Medium Medium
Forcer Weight Heaviest Lightest Moderate
Linear Motor Type Comparison [2]
Hannes Daepp
Components of a “Complete” Linear
Motor System [3]
1. Motor components
2. Base/Bearings
3. Servo controller/feedback
elements
• Typical sensors include Hall
Effect (for position) and thermal
sensors
1. Cable management
Hannes Daepp
Sample Pricing
$3529
 Trilogy T1S Ironless linear
motor
 110V, 1 pole motor
 Single bearing rail
 ~12’’ travel
 magnetic encoder
 Peak Velocity = 7 m/s
 Resolution = 5μm
Hannes Daepp
Applications[3],[5],[6]
 Small Linear Motors
 Packaging and Material Handling
 Automated Assembly
 Reciprocating compressors and
alternators
 Large Linear Induction Machines
(3 phase)
 Transportation
 Materials handling
 Extrusion presses
References
[1] S. Cetinkunt, Mechatronics, John Wiley & Sons, Inc., Hoboken 2007.
[2] J. Barrett, T. Harned, J. Monnich, Linear Motor Basics, Parker
Hannifin Corporation,
http://www.parkermotion.com/whitepages/linearmotorarticle.pdf
[3] Trilogy Linear Motor & Linear Motor Positioners, Parker Hannifin
Corporation, 2008,
http://www.parkermotion.com/pdfs/Trilogy_Catalog.pdf
[4] Rockwell Automation,
http://www.rockwellautomation.com/anorad/
products/linearmotors/questions.html
[5] J. Marsh, Motor Parameters Application Note, Parker-Trilogy Linear
Motors, 2003. http://www.parkermotion.com/whitepages/
Linear_Motor_Parameter_Application_Note.pdf
[6] Greg Paula, Linear motors take center stage, The American Society
of Mechanical Engineers, 1998.
References (continued)
54
 http://www.physclips.unsw.edu.au/jw/electricmotors.h
tml
 http://www.speedace.info/solar_car_motor_and_drivet
rain.htm
 http://www.allaboutcircuits.com/vol_2/chpt_13/1.html
 http://www.tpub.com/neets/book5/18d.htm single
phase induction motor
 http://www.stefanv.com/rcstuff/qf200212.html
Brushless DC motors
 https://www.geckodrive.com/upload/Step_motor_basic
s.pdf
 http://www.solarbotics.net/library/pdflib/pdf/motorbas
.pdf
THANK YOU

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Slide pertemuan 11.txt

  • 3. 3
  • 4. 4
  • 5. 5
  • 6. 6
  • 7. 7
  • 8. 8 Electric Motor Basic Principles  Interaction between magnetic field and current carrying wire produces a force  Opposite of a generator Sean DeHart
  • 9. 9 Conventional (Brushed) DC Motors  Permanent magnets for outer stator  Rotating coils for inner rotor  Commutation performed with metal contact brushes and contacts designed to reverse the polarity of the rotor as it reaches horizontal Sean DeHart
  • 10. 10 2 pole brushed DC motor commutation Sean DeHart
  • 11. 11 Conventional (Brushed) DC Motors  Common Applications: Small/cheap devices such as toys, electric tooth brushes, small drills Lab 3  Pros: Cheap, simple Easy to control - speed is governed by the voltage and torque by the current through the armature  Cons: Mechanical brushes - electrical noise, arcing, sparking, friction, wear, inefficient, shorting Sean DeHart
  • 12. 12 DC Motor considerations  Back EMF - every motor is also a generator  More current = more torque; more voltage = more speed  Load, torque, speed characteristics  Shunt-wound, series-wound (aka universal motor), compound DC motors Sean DeHart
  • 13. 13 Brushless DC Motors  Essential difference - commutation is performed electronically with controller rather than mechanically with brushes Sean DeHart
  • 14. 14 Brushless DC Motor Commutation  Commutation is performed electronically using a controller (e.g. HCS12 or logic circuit) Similarity with stepper motor, but with less # poles Needs rotor positional closed loop feedback: hall effect sensors, back EMF, photo transistors Sean DeHart
  • 15. 15 Delta               Wye BLDC (3-Pole) Motor Connections  Has 3 leads instead of 2 like brushed DC  Delta (greater speed) and Wye (greater torque) stator windings Sean DeHart
  • 16. 16 Brushless DC Motors  Applications CPU cooling fans CD/DVD Players Electric automobiles  Pros (compared to brushed DC) Higher efficiency Longer lifespan, low maintenance Clean, fast, no sparking/issues with brushed contacts  Cons Higher cost More complex circuitry and requires a controller Sean DeHart
  • 17. AC Motors Two main types of AC motor, Synchronous and Induction. Synchronous motors supply power to both the rotor and the stator, where induction motors only supply power to the stator coils, and rely on induction to generate torque. 17Sean DeHart
  • 18. 18 AC Induction Motors (3 Phase)  Use poly-phase (usually 3) AC current to create a rotating magnetic field on the stator  This induces a magnetic field on the rotor, which tries to follow stator - slipping required to produce torque  Workhorses of the industry - high powered applications Sean DeHart
  • 19. AC induction Motors Induction motors only supply current to the stator, and rely on a second induced current in the rotor coils. This requires a relative speed between the rotating magnetic field and the rotor. If the rotor somehow matches or exceeds the magnetic field speed, there is condition called slip. Slip is required to produce torque, if there is no slip, there is no difference between the induced pole and the powered pole, and therefore no torque on the shaft. 19Sean DeHart
  • 20. Synchronous AC Motors Current is applied to both the Rotor and the Stator. This allows for precise control (stepper motors), but requires mechanical brushes or slip rings to supply DC current to the rotor. There is no slip since the rotor does not rely on induction to produce torque. 20Sean DeHart
  • 21. Stepper Motor A stepper motor is an electromechanical device which converts electrical pulses into discrete mechanical movements. The shaft or spindle of a stepper motor rotates in discrete step increments when electrical command pulses are applied to it in the proper sequence. Smriti Chopra
  • 22. Main features The sequence of the applied pulses is directly related to the direction of motor shafts rotation. The speed of the motor shafts rotation is directly related to the frequency of the input pulses. The length of rotation is directly related to the number of input pulses applied. Smriti Chopra
  • 23. Stepper Motor Characteristics   Open loop The motors response to digital input pulses provides open-loop control, making the motor simpler and less costly to control.     Brushless    Very reliable since there are no contact brushes in the motor. Therefore the life of the motor is simply dependant on the life of the bearing. Incremental steps/changes The rotation angle of the motor is proportional to the input pulse. Speed increases -> torque decreases Smriti Chopra
  • 24. Torque vs. Speed Torque varies inversely with speed. Current is proportional to torque. Torque ∞ means Current ∞,→ → which leads to motor damage. Torque thus needs to be limited to rated value of motor. Smriti Chopra
  • 25. Disadvantages of stepper motors There are two main disadvantages of stepper motors: Resonance can occur if not properly controlled. This can be seen as a sudden loss or drop in torque at certain speeds which can result in missed steps or loss of synchronism. It occurs when the input step pulse rate coincides with the natural oscillation frequency of the rotor. Resonance can be minimised by using half stepping or microstepping. Not easy to operate at extremely high speeds. 25
  • 26. Working principle Stepper motors consist of a permanent magnet rotating shaft, called the rotor, and electromagnets on the stationary portion that surrounds the motor, called the stator. When a phase winding of a stepper motor is energized with current, a magnetic flux is developed in the stator. The direction of this flux is determined by the “Right Hand Rule”. Smriti Chopra
  • 27. At position 1, the rotor is beginning at the upper electromagnet, which is currently active (has voltage applied to it). To move the rotor clockwise (CW), the upper electromagnet is deactivated and the right electromagnet is activated, causing the rotor to move 90 degrees CW, aligning itself with the active magnet. This process is repeated in the same manner at the south and west electromagnets until we once again reach the starting position. Smriti Chopra
  • 28. Understanding resolution Resolution is the number of degrees rotated per step. Step angle = 360/(NPh * Ph) = 360/N NPh = Number of equivalent poles per phase = number of rotor poles. Ph = Number of phases. N = Total number of poles for all phases together. Example: for a three winding motor with a rotor having 4 teeth, the resolution is 30 degrees. Smriti Chopra
  • 29. Two phase stepper motors There are two basic winding arrangements for the electromagnetic coils in a two phase stepper motor: bipolar and unipolar. unipolar bipolar Smriti Chopra
  • 30. A unipolar stepper motor has two windings per phase, one for each direction of magnetic field. In this arrangement a magnetic pole can be reversed without switching the direction of current. Bipolar motors have a single winding per phase. The current in a winding needs to be reversed in order to reverse a magnetic pole. Bipolar motors have higher torque but need more complex driver circuits. Main difference Smriti Chopra
  • 31. Stepping modes Wave Drive (1 phase on) A1 – B2 – A2 – B1 (25% of unipolar windings , 50% of bipolar) Full Step Drive (2 phases on) A1B2 – B2A2 – A2B1 – B1A1 (50% of unipolar windings , full bipolar windings utilization) Half Step Drive (1 & 2 phases on) A1B2 – B2 – B2A2 – A2 ---- (increases resolution) Microstepping (Continuously varying motor currents) A microstep driver may split a full step into as many as 256 microsteps. Smriti Chopra
  • 32. Types of Stepper Motors There are three main types of stepper motors: Variable Reluctance stepper motor Permanent Magnet stepper motor Hybrid Synchronous stepper motor Smriti Chopra
  • 33. This type of motor consists of a soft iron multi-toothed rotor and a wound stator. When the stator windings are energized with DC Current, the poles become magnetized. Rotation occurs when the rotor teeth are attracted to the energized stator poles. Variable Reluctance motor Smriti Chopra
  • 34. Permanent Magnet motor The rotor no longer has teeth as with the VR motor. Instead the rotor is magnetized with alternating north and south poles situated in a straight line parallel to the rotor shaft. These magnetized rotor poles provide an increased magnetic flux intensity and because of this the PM motor exhibits improved torque characteristics when compared with the VR type. Smriti Chopra
  • 35. Hybrid Synchronous motor The rotor is multi-toothed like the VR motor and contains an axially magnetized concentric magnet around its shaft. The teeth on the rotor provide an even better path which helps guide the magnetic flux to preferred locations in the air gap. Smriti Chopra
  • 36. Applications Stepper motors can be a good choice whenever controlled movement is required. They can be used to advantage in applications where you need to control rotation angle, speed, position and synchronism. These include  printers  plotters  medical equipment  fax machines  automotive and scientific equipment etc. Smriti Chopra
  • 38. Hannes Daepp Basics of Linear Motors [1],[4] I Analogous to Unrolled DC Motor • Force (F) is generated when the current (I) (along vector L) and the flux density (B) interact • F = LI x B
  • 39. Hannes Daepp Linear Motors in Action  http://www.parkermotion.com/video/Braas_Trilogy_T3E_Video.MPG
  • 40. Hannes Daepp Analysis of Linear Motors [1],[5] Analysis is similar to that of rotary machines Linear dimension and displacements replace angular ones Forces replace torques Commutation cycle is distance between two consecutive pole pairs instead of 360 degrees
  • 41. Hannes Daepp Benefits of Linear Motors [2] High Maximum Speed Limited primarily by bus voltage, control electronics High Precision Accuracy, resolution, repeatability limited by feedback device, budget Zero backlash: No mechanical transmission components. Fast Response Response rate can be over 100 times that of a mechanical transmission  faster accelerations, settling time (more throughput) Stiffness No mechanical linkage, stiffness depends mostly on gain & current Durable Modern linear motors have few/no contacting parts  no wear
  • 42. Hannes Daepp Downsides of Linear Motors [2] Cost Low production volume (relative to demand) High price of magnets Linear encoders (feedback) are much more expensive than rotary encoders, cost increases with length Higher Bandwidth Drives and Controls Lower force per package size Heating issues Forcer is usually attached to load  I2 R losses are directly coupled to load No (minimal) Friction No automatic brake
  • 43. Hannes Daepp Components of Linear Motors [2],[3] Forcer (Motor Coil) Windings (coils) provide current (I) Windings are encapsulated within core material Mounting Plate on top Usually contains sensors (hall effect and thermal) Magnet Rail Iron Plate / Base Plate Rare Earth Magnets of alternating polarity provide flux (B) Single or double rail F = lI x B
  • 44. Hannes Daepp Types of Linear Motors [1],[2],[3] Iron Core  Coils wound around teeth of laminations on forcer Ironless Core  Dual back iron separated by spacer  Coils held together with epoxy Slotless  Coil and back iron held together with epoxy
  • 45. Hannes Daepp Linear Motor Types: Iron Core [1],[2] Distinguishing Feature  Copper windings around forcer laminations over a single magnet rail Advantages:  Highest force available per unit volume  Efficient Cooling  Lower cost Disadvantages:  High attractive force between forcer & magnet track  Cogging: iron forcer affects thrust force as it passes over each magnet (aka velocity ripple)
  • 46. Hannes Daepp Distinguishing Feature  Forcer constructed of wound coils held together with epoxy and running between two rails (North and South)  Also known as “Aircore” or “U-channel” motors Advantages:  No attractive forces in forcer  No Cogging  Low weight forcer - No iron means higher accel/decel rates Top View Forcer Mounting Plate Rare Earth Magnets Horseshoe Shaped backiron Winding, held by epoxy Hall Effect and Thermal Sensors in coil Front View Linear Motor Types: Ironless [1],[2] Disadvantages:  Low force per package size  Lower Stiffness; limited max load without improved structure  Poor heat dissipation  Higher cost (2x Magnets!)
  • 47. Hannes Daepp Distinguishing Feature  Mix of ironless and iron core: coils with back iron contained within aluminum housing over a single magnet rail Advantages over ironless:  Lower cost (1x magnets)  Better heat dissipation  Structurally stronger forcer  More force per package size Advantages over iron core:  Lighter weight and lower inertia forcer  Lower attractive forces  Less cogging Side View Front View Back iron Mounting plate Coil assemblyThermal sensor Rare Earth Magnets Iron plate Linear Motor Types: Slotless [1],[2]
  • 48. Hannes Daepp Disadvantages  Some attractive force and cogging  Less efficient than iron core and ironless - more heat to do the same job Side View Front View Back iron Mounting plate Coil assemblyThermal sensor Rare Earth Magnets Iron plate Linear Motor Types: Slotless [2],[3]
  • 49. Hannes Daepp Linear Brushless DC Motor Type Feature Iron Core Ironless Slotless Attraction Force Most None Moderate Cost Medium High Lowest Force Cogging Highest None Medium Power Density Highest Medium Medium Forcer Weight Heaviest Lightest Moderate Linear Motor Type Comparison [2]
  • 50. Hannes Daepp Components of a “Complete” Linear Motor System [3] 1. Motor components 2. Base/Bearings 3. Servo controller/feedback elements • Typical sensors include Hall Effect (for position) and thermal sensors 1. Cable management
  • 51. Hannes Daepp Sample Pricing $3529  Trilogy T1S Ironless linear motor  110V, 1 pole motor  Single bearing rail  ~12’’ travel  magnetic encoder  Peak Velocity = 7 m/s  Resolution = 5μm
  • 52. Hannes Daepp Applications[3],[5],[6]  Small Linear Motors  Packaging and Material Handling  Automated Assembly  Reciprocating compressors and alternators  Large Linear Induction Machines (3 phase)  Transportation  Materials handling  Extrusion presses
  • 53. References [1] S. Cetinkunt, Mechatronics, John Wiley & Sons, Inc., Hoboken 2007. [2] J. Barrett, T. Harned, J. Monnich, Linear Motor Basics, Parker Hannifin Corporation, http://www.parkermotion.com/whitepages/linearmotorarticle.pdf [3] Trilogy Linear Motor & Linear Motor Positioners, Parker Hannifin Corporation, 2008, http://www.parkermotion.com/pdfs/Trilogy_Catalog.pdf [4] Rockwell Automation, http://www.rockwellautomation.com/anorad/ products/linearmotors/questions.html [5] J. Marsh, Motor Parameters Application Note, Parker-Trilogy Linear Motors, 2003. http://www.parkermotion.com/whitepages/ Linear_Motor_Parameter_Application_Note.pdf [6] Greg Paula, Linear motors take center stage, The American Society of Mechanical Engineers, 1998.
  • 54. References (continued) 54  http://www.physclips.unsw.edu.au/jw/electricmotors.h tml  http://www.speedace.info/solar_car_motor_and_drivet rain.htm  http://www.allaboutcircuits.com/vol_2/chpt_13/1.html  http://www.tpub.com/neets/book5/18d.htm single phase induction motor  http://www.stefanv.com/rcstuff/qf200212.html Brushless DC motors  https://www.geckodrive.com/upload/Step_motor_basic s.pdf  http://www.solarbotics.net/library/pdflib/pdf/motorbas .pdf

Editor's Notes

  1. left: current carrying wire F=BIL pair of force produces torque - spins the rotor    right: electromagnet with metal core wrapped by wire coils coil creates N and S poles - becomes attracted to S and N poles on stator, respectively  the idea, is then how to create a dynamically changing magnetic flux to keep the rotor spinning constantly faraday's law concerning generators: generated emf = rate of change of magnetic flux
  2. 2 pole DC electric motor Direct Current a better picture of rotation/commutation next slide
  3. important to note that with this simple 2 pole motor, when rotor rotates 90 degrees from this picture, there will be 0 torque. Unable to start from rest at that 90deg position in practice, a real DC motor use more than 2 poles to eliminate - zero torque zone, and shorting of battery
  4. mechanical brushes could be metallic or carbon
  5. under no load conditions, motor will rotate at a speed such that the back emf equals the applied voltage plus voltage drop across armature    generally highest torque at zero speed, zero torque at max speed  increase current to increase torque increase voltage to increase speed    shunt wound, series wound DC motors: Here, the stator is an electromagnet instead of permanent magnet.   shunt has stator and armature connected in parallel. series has stators and armature connected in series.  Has different loading characteristics    series wound DC is also known as universal motor and can run on both AC and DC because both stator and rotor polarity can be switched
  6. Brushed DC motor  - 'conventional'/'inrunner' configuration:  flipped inside out - stator is now coil, rotor is permanent magnet that spins on the inside typically less torque, but high RPM  'outrunner' configuration - rotor spins on the outside around stator. typically high torque but lower RPM   Energize the stator electromagnet coils sequentially (very much like a stepper motor) to make the rotor rotate
  7. How to know when to energize coils?  cannot do this in open loop like stepper due to smaller number of poles on stator; needs feedback    2 ways to sense rotor position: -hall effect sensor (detects magnetic fields) -sensorless (back emf on the un-energized coils) -photo transistors (encoders, lab3 slot and detector)        
  8. left diagram (delta): sequentially energize each of the 3 leads to make rotor turn if more poles/windings on stator, typically still arranged into 3 groups - hence still 3 leads   wye - greater torque at low speeds delta - greater speed    delta, wye in AC transformers - neutral wires -  phase to neutral voltages available for wye.  only phase to phase voltage available for delta 
  9. There are also single phase - require external starter       AC current through the stator windings creates a time varying magnetic field. This induces an emf across the conductive rotor (often a 'squirrel cage' This makes the rotor a magnet, which then interacts with the magnetic field of the stator. The goal is to make a rotating magnetic field with the stator.Induction motors require (slip) workhorse of industry - rugged construction; no brushes to wear out - reliable, low maintenance
  10. Commutation cycle in rotary brushless motor is 360 degrees
  11. Typical max speeds: 3-5 m/s with 1 micron resolution, 5+ m/s (>200 ips) with less resolution Budget is main restraint on controller bandwidth Higher stiffness (spring rate), though limited by motor peak force, available current, and feedbakc resolution
  12. Linear encoders are usually around $500 for 100 mm travel encoder, cost increases with length. Rotary encoders are relatively inexpensive – tend to be under 100 dollars No mechanical reduction between motor and load, thus servo response (bandwidth) must be faster. Includes higher encoder bandwidth and servo update rates Linear motors are not compact force generators when compared to rotary motor with transmission offering mechanical advantage. Example 3/8” diam. Ball screw produces 100 lb of thrust, while 15 lb of linear thrust typically requires 2” x 1.5” cross section. Heat management techniques such as air and water cooling options (both common, popular) have to be applied Suppose it’s traveling at 3 m/s and loses power. Without resistance, it will quickly reach end of end of system, mechanical stops.
  13. Iron core: base plate with magnets, basically a brushless DC motor laid out. Magnetic back iron keeps it down by maintaining magnetic attraction to place Ironless: NO back iron. Slotless: Just one rail, often uses non-ferrous housing to support coil assembly (so that it’s not limited purely to epoxy, but isn’t magnetic)
  14. -- Highest force per unit volume is because laminations concentrate flux field -- iron forcer also aids in heat dissipation. Cooling tubes can be routed through laminations to improve thermal managment -- only 1 row of magnets  lower cost Disadvantages: -- Since the forcer consists of iron, it is attracted to the permanent magnets. Bearings are used to support the force. Can be up to 10 x thrust force, meaning that choice of bearings is critical. -- “Cogging: Since the forcer is made of iron and it passes over magnets, there is a variation in the thrust force as it passes each magnet. This is referred to as cogging and affects low speed smoothness (velocity ripple) [8]”
  15. -- No back iron in forcer, but is usually topped with an aluminum bar for mounting the load and for heat removal Advantages: -- No attractive forces (no iron in forcer), so no additional forces on bearings. Motor is also easier to handle, install -- ironless forcer  no cogging. Great for extreme velocity control. Usually used with air bearings due to their “ultra-smooth characteristics” Disadvantages: -- since forcer is just coils with epoxy below plate, heat must leave the coil to aluminum plate via coil or through the air gap in magnet rail. High thermal resistance makes heat dissipation an issue. -- Weak structure relative to iron core, since forcer is made of coils and epoxy (as opposed to iron). Also limits max sizes and forces to which these motors can be manufactured without adding additional structural members -- Double rail, along with thermal and structural limitations, contributes to lower force per package size
  16. Hybrid between iron core and ironless linear motor designs v. Ironless -- less weight than ironless. Higher accelerations -- Housing provides considerably improved heat dissipation -- housing makes structure better than ironless; can handle larger loads -- force per package size between ironless and iron core. Better thermal management also means that it can handle higher currents than ironless and thus generate higher forces v. Iron Core -- Light weight forcer (aluminum v. iron) means higher throughput in light load applications -- back iron causes 5-7 times less attractive force than with iron core -- larger magnetic gap between magnets and forcer backiron results in less cogging  better velocity control
  17. Hybrid between iron core and ironless linear motor designs
  18. 8-pole 117’’ travel dual rail ~$15,000 (Trilogy)
  19. Packaging: Particular notice in semiconductor industry, where precision is critical and motions of under 1 micron are often desired Most widely known use of linear motors is in transportation Automotive indsutry has been quick to pick up on linear motors because it allows more flexibility – can simply change fixtures for different cars instead of customizing assembly to one vehicle [6]