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Overview
 DC Motors (Brushed and Brushless)
 Stepper Motors
Sean DeHart
3
Electric Motor Basic Principles
 Interaction between magnetic field and current
carrying wire produces a force
 Opposite of a generator
Sean DeHart
4
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
5
2 pole brushed DC motor commutation
Sean DeHart
6
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
7
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
8
Brushless DC Motors
 Essential difference - commutation is performed
electronically with controller rather than
mechanically with brushes
Sean DeHart
9
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
10
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
11
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
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.
16
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
 3phase induction motor-Not a variable speed motor
 1 Phase induction motor-Not self starting, poor power factor,
efficiency
Common single phase commutator motors are
1.Series motors
2.Universal motors
3.Repulsion motors
4.Repulsion –induction motors
If we connect normal dc series motor to ac what happens?
1. Torque developed is not constant Magnitude
2. Alternating flux induce eddy currents causing heat and there by
loss
3. No inductive coupling between armature and field since they
are placed in quadrature
4. Sparking in brushes is more due to transformer emf induced
5. Due to large voltage drop speed reduced
6. Starting Torque is low, low pf
Modification needed for ac series motor.
1. To reduce eddy current loss-Laminations used
2. To reduce reactance-series field should contains less number of
turns
3. To improve torque no. of armature conductors should be large
4. To reduce reactance compensating winding should be used
5. Operating voltage kept low to reduce inductance
6. Reduce frequency to reduce inductance
7. Interpoles to reduce armature resistance leads
Construction
Changes should be employed to work in both ac and dc
Operation
When motor is connected to an a.c. supply, the same alternating
current flows
through the field and armature windings.
The field winding produces an alternating flux that reacts with the
current flowing in the armature to produce a torque.
Since both armature current and flux reverse simultaneously, the
torque always acts in the same direction.
It may be noted that no rotating flux is produced in this type of
machines; the principle of operation is the same as that of a d.c. series
motor.
Characteristics
The operating characteristics of an a.c. series motor are similar to those
of a d.c. series motor.
(i) The speed increases to a high value with a decrease in load. In very
small series motors, the losses are usually large enough at no load that
limit the speed to a definite value (1500 - 15,000 r.p.m.).
(ii) The motor torque is high for large armature currents, thus giving a
high
starting torque.
(iii) At full-load, the power factor is about 90%. However, at starting or
when
carrying an overload, the power factor is lower
Applications
The fractional horsepower a.c. series motors have high-speed (and
corresponding small size) and large starting torque. They can,
therefore, be used
to drive:
(a) high-speed vacuum cleaners (b) sewing machines
(c) electric shavers (d) drills
(e) machine tools etc.
A repulsion motor is similar to an a.c. series motor except that:
(i) brushes are not connected to supply but are short-circuited -
currents are induced in the armature conductors by transformer
action.
(ii) the field structure has non-salient pole construction.
By adjusting the position of short-circuited brushes on the
commutator, the starting torque can be developed in the motor
Construction
The field of stator winding is wound like the main winding of a split-phase
motor and is connected directly to a single-phase source.
The armature or rotor is similar to a d.c. motor armature with drum type
winding connected to a commutator
However, the brushes are not connected to supply but are connected to
each other or short-circuited.
Short-circuiting the brushes effectively makes the rotor into a type of
squirrel cage.
The major difficulty with an ordinary single-phase induction motor is the
low starting torque.
It has also better power factor than the conventional single-phase motor.
Construction
Principle of operation
The total armature torque in a repulsion motor can be shown to be
Ta = sin 2α
where α = angle between brush axis and stator field axis
For maximum torque, 2α = 90° or α = 45°
Thus adjusting α to 45° at starting, maximum torque can be obtained
during the starting period. However, α has to be adjusted to give a
suitable running speed.
Characteristics
(i) The repulsion motor has characteristics very similar to those of an
a.c. series motor i.e., it has a high starting torque and a high speed at
no load.
(ii) The speed which the repulsion motor develops for any given load
will depend upon the position of the brushes.
(iii) In comparison with other single-phase motors, the repulsion
motor has a high starring torque and relatively low starting current.
Sometimes the action of a repulsion motor is combined with that of a
single phase induction motor to produce repulsion-start induction-run
motor (also called repulsion-start motor).
The machine is started as a repulsion motor with a corresponding high
starting torque.
At some predetermined speed, a centrifugal device short-circuits the
commutator so that the machine then operates as a single-phase
induction motor.
This motor has the same general construction of a repulsion motor.
The only difference is that it is equipped with a centrifugal device fitted
on the armature shaft.
When the motor reaches 75% of its full pinning speed, the centrifugal
device forces a short-circuiting ring to come in contact with the inner
surface of the commutator.
This short-circuits all the commutator bars.
The rotor then resembles squirrel-cage type and the motor runs as a
single-phase induction motor.
At the same time, the centrifugal device raises the brushes from the
commutator which reduces the wear of the brushes and commutator as
well as makes the operation quiet.
Characteristics
(i) The starting torque is 2.5 to 4.5 times the full-load torque and the
starting
current is 3.75 times the full-load value.
(ii) Due to their high starting torque, repulsion-motors were used to
operate
devices such as refrigerators, pumps, compressors etc.
However, they posed a serious problem of maintenance of brushes,
commutator
arid the centrifugal device.
The repulsion-induction motor produces a high starting torque entirely
due to repulsion motor action. When running, it functions through a
combination of induction-motor and repulsion motor action.
Construction
It consists of a stator and a rotor (or armature).
(i) The stator carries a single distributed winding fed from single-phase supply.
(ii) The rotor is provided with two independent windings placed one inside the
other.
The inner winding is a squirrel-cage winding with rotor bars
permanently short-circuited. Placed over the squirrel cage winding is a
repulsion commutator armature winding.
The repulsion winding is connected to a commutator on which ride short-
circuited brushes. There is no centrifugal device and the repulsion winding
functions at all times.
Operation
(i) When single-phase supply is given to the stator winding, the repulsion
winding (i.e., outer winding) is active. Consequently, the motor starts as a
repulsion motor with a corresponding high starting torque.
(ii) As the motor speed increases, the current shifts from the outer to
inner
winding due to the decreasing impedance of the inner winding with
increasing speed. Consequently, at running speed, the squirrel cage
winding carries the greater part of rotor current.
This shifting of repulsion motor action to induction-motor action is thus
achieved without any switching arrangement.
Characteristics
(i) The no-load speed of a repulsion-induction motor is somewhat above
the
synchronous speed because of the effect of repulsion winding. However,
the speed at full-load is slightly less than the synchronous speed as in an
induction motor.
(ii) The speed regulation of the motor is about 6%.
(iii) The starting torque is 2.25 to 3 times the full-load torque; the lower
value
being for large motors. The starting current is 3 to 4 times the full-load
current.
This type of motor is used for applications requiring a high starting
torque with
Very small single-phase motors have been developed which run at true
synchronous speed. They do not require d.c. excitation for the rotor.
Because of these characteristics, they are called unexcited single-phase
synchronous motors.
The most commonly used types are:
(i) Reluctance motors (ii) Hysteresis motors
The efficiency and torque-developing ability of these motors is low; The
output of most of the commercial motors is only a few watts
It is a single-phase synchronous motor which does not require d.c.
excitation to the rotor.
Its operation is based upon the following principle:
Whenever a piece of ferromagnetic material is located in a magnetic field;
a force is exerted on the material, tending to align the material so that
reluctance of the magnetic path that passes through the material is
minimum.
Construction
(i) a stator carrying a single-phase winding along with an auxiliary
winding to produce a synchronous-revolving magnetic field.
(ii) a squirrel-cage rotor having unsymmetrical magnetic construction.
This is achieved by symmetrically removing some of the teeth from the
squirrel cage rotor to produce salient poles on the rotor.
The salient poles created on the rotor must be equal to the poles on the
stator.
Note that rotor salient poles offer low reluctance to the stator flux and,
therefore, become strongly magnetized.
Operation
(i) When single-phase stator having an auxiliary winding is energized, a
synchronously-revolving field is produced. The motor starts as a standard
squirrel-cage induction motor and will accelerate to near its synchronous
speed.
(ii) As the rotor approaches synchronous speed, the rotating stator flux
will
exert reluctance torque on the rotor poles tending to align the salient-
pole
axis with the axis of the rotating field. The rotor assumes a position where
its salient poles lock with the poles of the revolving field
(ii)) Consequently, the motor will continue to run at the speed of
revolving flux i.e., at the synchronous speed.
Operation
(iii) When we apply a mechanical load, the rotor poles fall slightly behind
the
stator poles, while continuing to turn at synchronous speed.
As the load on the motor is increased, the mechanical angle between the
poles increases progressively.
Nevertheless, magnetic attraction keeps the rotor locked to the rotating
flux. If the load is increased beyond the amount under which the
reluctance torque can maintain synchronous speed
Characteristics
(i) These motors have poor torque, power factor and efficiency.
(ii) These motors cannot accelerate high-inertia loads to synchronous
speed.
(iii)The pull-in and pull-out torques of such motors are weak.
Despite the above drawbacks, the reluctance motor is cheaper than any
other
type of synchronous motor. They are widely used for constant-speed
applications such as timing devices, signaling devices etc
It is a single-phase motor whose operation depends upon the hysteresis
effect i.e., magnetization produced in a ferromagnetic material lags
behind the magnetizing force.
Construction
(i) a stator designed to produce a synchronously-revolving field from a
single-phase supply. This is accomplished by using permanent-split
capacitor type construction. Consequently, both the windings (i.e.,
starting
as well as main winding) remain connected in the circuit during running
operation as well as at starting. The value of capacitance is so adjusted as
to
result in a flux revolving at synchronous speed.
(ii) a rotor consisting of a smooth cylinder of magnetically hard steel,
without winding or teeth.
Operation
(i) When the stator is energized from a single-phase supply, a
synchronously revolving field (assumed in anti-clockwise direction) is
produced due to split-phase operation.
(ii) The revolving stator flux magnetizes the rotor. Due to hysteresis
effect, the axis of magnetization of rotor will lag behind the axis of stator
field by
hysteresis lag angle ,the rotor and stator poles are locked. If the rotor is
stationary, the starting torque produced is given by:
Operation
From now onwards, the rotor accelerates to synchronous speed with a
uniform torque.
(iii) After reaching synchronism, the motor continues to run at
synchronous speed and adjusts its torque angle so as to develop the
torque required by the load.
Characteristics
(i) A hysteresis motor can synchronize any load which it can accelerate,
no
matter how great the inertia. It is because the torque is uniform from
standstill to synchronous speed.
(ii) Since the rotor has no teeth or salient poles or winding, a hysteresis
motor
is inherently quiet and produces smooth rotation of the load.
(iii) The rotor takes on the same number of poles as the stator field. Thus
by
changing the number of stator poles through pole-changing connections,
we can get a set of synchronous speeds for the motor.
Applications
Due to their quiet operation and ability to drive high-inertia toads,
hysteresis
motors are particularly well suited for driving
(i)electric clocks
(ii)Timing devices
(iii) tape-decks
(iv)from-tables and other precision audio-equipment.

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Special motors

  • 1.
  • 2. 2 Overview  DC Motors (Brushed and Brushless)  Stepper Motors Sean DeHart
  • 3. 3 Electric Motor Basic Principles  Interaction between magnetic field and current carrying wire produces a force  Opposite of a generator Sean DeHart
  • 4. 4 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
  • 5. 5 2 pole brushed DC motor commutation Sean DeHart
  • 6. 6 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
  • 7. 7 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
  • 8. 8 Brushless DC Motors  Essential difference - commutation is performed electronically with controller rather than mechanically with brushes Sean DeHart
  • 9. 9 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
  • 10. 10 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
  • 11. 11 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
  • 12. 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
  • 13. 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
  • 14. 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
  • 15. 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
  • 16. 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. 16
  • 17. 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
  • 18. 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
  • 19. 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
  • 20. 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
  • 21. 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
  • 22. 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
  • 23. 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
  • 24. 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
  • 25. 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
  • 26. 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
  • 27. 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
  • 28.  3phase induction motor-Not a variable speed motor  1 Phase induction motor-Not self starting, poor power factor, efficiency Common single phase commutator motors are 1.Series motors 2.Universal motors 3.Repulsion motors 4.Repulsion –induction motors
  • 29. If we connect normal dc series motor to ac what happens? 1. Torque developed is not constant Magnitude 2. Alternating flux induce eddy currents causing heat and there by loss 3. No inductive coupling between armature and field since they are placed in quadrature 4. Sparking in brushes is more due to transformer emf induced 5. Due to large voltage drop speed reduced 6. Starting Torque is low, low pf
  • 30. Modification needed for ac series motor. 1. To reduce eddy current loss-Laminations used 2. To reduce reactance-series field should contains less number of turns 3. To improve torque no. of armature conductors should be large 4. To reduce reactance compensating winding should be used 5. Operating voltage kept low to reduce inductance 6. Reduce frequency to reduce inductance 7. Interpoles to reduce armature resistance leads
  • 31. Construction Changes should be employed to work in both ac and dc
  • 32. Operation When motor is connected to an a.c. supply, the same alternating current flows through the field and armature windings. The field winding produces an alternating flux that reacts with the current flowing in the armature to produce a torque. Since both armature current and flux reverse simultaneously, the torque always acts in the same direction. It may be noted that no rotating flux is produced in this type of machines; the principle of operation is the same as that of a d.c. series motor.
  • 33. Characteristics The operating characteristics of an a.c. series motor are similar to those of a d.c. series motor. (i) The speed increases to a high value with a decrease in load. In very small series motors, the losses are usually large enough at no load that limit the speed to a definite value (1500 - 15,000 r.p.m.). (ii) The motor torque is high for large armature currents, thus giving a high starting torque. (iii) At full-load, the power factor is about 90%. However, at starting or when carrying an overload, the power factor is lower
  • 34. Applications The fractional horsepower a.c. series motors have high-speed (and corresponding small size) and large starting torque. They can, therefore, be used to drive: (a) high-speed vacuum cleaners (b) sewing machines (c) electric shavers (d) drills (e) machine tools etc.
  • 35. A repulsion motor is similar to an a.c. series motor except that: (i) brushes are not connected to supply but are short-circuited - currents are induced in the armature conductors by transformer action. (ii) the field structure has non-salient pole construction. By adjusting the position of short-circuited brushes on the commutator, the starting torque can be developed in the motor
  • 36. Construction The field of stator winding is wound like the main winding of a split-phase motor and is connected directly to a single-phase source. The armature or rotor is similar to a d.c. motor armature with drum type winding connected to a commutator However, the brushes are not connected to supply but are connected to each other or short-circuited. Short-circuiting the brushes effectively makes the rotor into a type of squirrel cage. The major difficulty with an ordinary single-phase induction motor is the low starting torque. It has also better power factor than the conventional single-phase motor.
  • 39. The total armature torque in a repulsion motor can be shown to be Ta = sin 2α where α = angle between brush axis and stator field axis For maximum torque, 2α = 90° or α = 45° Thus adjusting α to 45° at starting, maximum torque can be obtained during the starting period. However, α has to be adjusted to give a suitable running speed.
  • 40. Characteristics (i) The repulsion motor has characteristics very similar to those of an a.c. series motor i.e., it has a high starting torque and a high speed at no load. (ii) The speed which the repulsion motor develops for any given load will depend upon the position of the brushes. (iii) In comparison with other single-phase motors, the repulsion motor has a high starring torque and relatively low starting current.
  • 41. Sometimes the action of a repulsion motor is combined with that of a single phase induction motor to produce repulsion-start induction-run motor (also called repulsion-start motor). The machine is started as a repulsion motor with a corresponding high starting torque. At some predetermined speed, a centrifugal device short-circuits the commutator so that the machine then operates as a single-phase induction motor.
  • 42. This motor has the same general construction of a repulsion motor. The only difference is that it is equipped with a centrifugal device fitted on the armature shaft. When the motor reaches 75% of its full pinning speed, the centrifugal device forces a short-circuiting ring to come in contact with the inner surface of the commutator. This short-circuits all the commutator bars. The rotor then resembles squirrel-cage type and the motor runs as a single-phase induction motor. At the same time, the centrifugal device raises the brushes from the commutator which reduces the wear of the brushes and commutator as well as makes the operation quiet.
  • 43. Characteristics (i) The starting torque is 2.5 to 4.5 times the full-load torque and the starting current is 3.75 times the full-load value. (ii) Due to their high starting torque, repulsion-motors were used to operate devices such as refrigerators, pumps, compressors etc. However, they posed a serious problem of maintenance of brushes, commutator arid the centrifugal device.
  • 44. The repulsion-induction motor produces a high starting torque entirely due to repulsion motor action. When running, it functions through a combination of induction-motor and repulsion motor action.
  • 45. Construction It consists of a stator and a rotor (or armature). (i) The stator carries a single distributed winding fed from single-phase supply. (ii) The rotor is provided with two independent windings placed one inside the other. The inner winding is a squirrel-cage winding with rotor bars permanently short-circuited. Placed over the squirrel cage winding is a repulsion commutator armature winding. The repulsion winding is connected to a commutator on which ride short- circuited brushes. There is no centrifugal device and the repulsion winding functions at all times.
  • 46. Operation (i) When single-phase supply is given to the stator winding, the repulsion winding (i.e., outer winding) is active. Consequently, the motor starts as a repulsion motor with a corresponding high starting torque. (ii) As the motor speed increases, the current shifts from the outer to inner winding due to the decreasing impedance of the inner winding with increasing speed. Consequently, at running speed, the squirrel cage winding carries the greater part of rotor current. This shifting of repulsion motor action to induction-motor action is thus achieved without any switching arrangement.
  • 47. Characteristics (i) The no-load speed of a repulsion-induction motor is somewhat above the synchronous speed because of the effect of repulsion winding. However, the speed at full-load is slightly less than the synchronous speed as in an induction motor. (ii) The speed regulation of the motor is about 6%. (iii) The starting torque is 2.25 to 3 times the full-load torque; the lower value being for large motors. The starting current is 3 to 4 times the full-load current. This type of motor is used for applications requiring a high starting torque with
  • 48. Very small single-phase motors have been developed which run at true synchronous speed. They do not require d.c. excitation for the rotor. Because of these characteristics, they are called unexcited single-phase synchronous motors. The most commonly used types are: (i) Reluctance motors (ii) Hysteresis motors The efficiency and torque-developing ability of these motors is low; The output of most of the commercial motors is only a few watts
  • 49. It is a single-phase synchronous motor which does not require d.c. excitation to the rotor. Its operation is based upon the following principle: Whenever a piece of ferromagnetic material is located in a magnetic field; a force is exerted on the material, tending to align the material so that reluctance of the magnetic path that passes through the material is minimum.
  • 50. Construction (i) a stator carrying a single-phase winding along with an auxiliary winding to produce a synchronous-revolving magnetic field. (ii) a squirrel-cage rotor having unsymmetrical magnetic construction. This is achieved by symmetrically removing some of the teeth from the squirrel cage rotor to produce salient poles on the rotor. The salient poles created on the rotor must be equal to the poles on the stator. Note that rotor salient poles offer low reluctance to the stator flux and, therefore, become strongly magnetized.
  • 51. Operation (i) When single-phase stator having an auxiliary winding is energized, a synchronously-revolving field is produced. The motor starts as a standard squirrel-cage induction motor and will accelerate to near its synchronous speed. (ii) As the rotor approaches synchronous speed, the rotating stator flux will exert reluctance torque on the rotor poles tending to align the salient- pole axis with the axis of the rotating field. The rotor assumes a position where its salient poles lock with the poles of the revolving field (ii)) Consequently, the motor will continue to run at the speed of revolving flux i.e., at the synchronous speed.
  • 52. Operation (iii) When we apply a mechanical load, the rotor poles fall slightly behind the stator poles, while continuing to turn at synchronous speed. As the load on the motor is increased, the mechanical angle between the poles increases progressively. Nevertheless, magnetic attraction keeps the rotor locked to the rotating flux. If the load is increased beyond the amount under which the reluctance torque can maintain synchronous speed
  • 53. Characteristics (i) These motors have poor torque, power factor and efficiency. (ii) These motors cannot accelerate high-inertia loads to synchronous speed. (iii)The pull-in and pull-out torques of such motors are weak. Despite the above drawbacks, the reluctance motor is cheaper than any other type of synchronous motor. They are widely used for constant-speed applications such as timing devices, signaling devices etc
  • 54. It is a single-phase motor whose operation depends upon the hysteresis effect i.e., magnetization produced in a ferromagnetic material lags behind the magnetizing force.
  • 55. Construction (i) a stator designed to produce a synchronously-revolving field from a single-phase supply. This is accomplished by using permanent-split capacitor type construction. Consequently, both the windings (i.e., starting as well as main winding) remain connected in the circuit during running operation as well as at starting. The value of capacitance is so adjusted as to result in a flux revolving at synchronous speed. (ii) a rotor consisting of a smooth cylinder of magnetically hard steel, without winding or teeth.
  • 56. Operation (i) When the stator is energized from a single-phase supply, a synchronously revolving field (assumed in anti-clockwise direction) is produced due to split-phase operation. (ii) The revolving stator flux magnetizes the rotor. Due to hysteresis effect, the axis of magnetization of rotor will lag behind the axis of stator field by hysteresis lag angle ,the rotor and stator poles are locked. If the rotor is stationary, the starting torque produced is given by:
  • 57. Operation From now onwards, the rotor accelerates to synchronous speed with a uniform torque. (iii) After reaching synchronism, the motor continues to run at synchronous speed and adjusts its torque angle so as to develop the torque required by the load.
  • 58. Characteristics (i) A hysteresis motor can synchronize any load which it can accelerate, no matter how great the inertia. It is because the torque is uniform from standstill to synchronous speed. (ii) Since the rotor has no teeth or salient poles or winding, a hysteresis motor is inherently quiet and produces smooth rotation of the load. (iii) The rotor takes on the same number of poles as the stator field. Thus by changing the number of stator poles through pole-changing connections, we can get a set of synchronous speeds for the motor.
  • 59. Applications Due to their quiet operation and ability to drive high-inertia toads, hysteresis motors are particularly well suited for driving (i)electric clocks (ii)Timing devices (iii) tape-decks (iv)from-tables and other precision audio-equipment.

Hinweis der Redaktion

  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