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    DC Motors

    EE 2802 Applied Electricity

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    Contents

    1. Introduction

    2. Construction

    3. Equivalent Circuit

    4. Operation

    5. Losses

    6. Starting a DC Motor7. Types of DC Motors

    8. Speed Control

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    Why DC motors are so common, when DCpower systems are rare?

    DC power systems are used in cars, trucks &aircrafts > use DC motors

    Wide variation in speed is possible(today induction motors with solidstate drive packages are mostlyused)

    1. Introduction

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    2. Construction

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    DC Motor Stator

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    Permanent magnets

    Can eliminate the power loss

    Improve the efficiency Disadvantage - constant flux

    Field windings around the poles

    Can control flux(by regulating the current in the winding)

    Stator

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    DC Motor Rotor

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    Rotating part is called the armature

    Made of highly permeable electricallyinsulated thin laminations;

    that are stacked together

    Electrical insulation reduces eddy currentlosses

    Slotsto house the armature windings

    Rotor

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    Commutator- made of copper segments- insulated from one another- converts alternating emf into a uni-

    directional voltage

    Electrical connection between external circuitand the armature coils

    - established using the stationarybrushes

    Rotor

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    2 types Lap windingWave winding

    Its the way the armature winding is connectedto the commutator

    Armature winding

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    Lap winding

    No. of brushes and the parallel paths betweenbrushes = No. of poles

    Used in low voltage, high current applications

    Armature winding

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    Wave winding

    No. of brushes and the parallel paths betweenbrushes = 2

    Used in high voltage, low current applications

    Armature winding

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    Armature circuit by Eaand Ra Field coils by Rfw and Nf Rfxexternal variable resistor to control the

    amount of filed circuit current

    3. Equivalent Circuit

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    A uniform magnetic field is created by the poles

    Armature conductors are connected to a DCpower source > carry current

    Current carrying conductors are now placed in amagnetic field

    Will experiences a force / torque

    Armature starts rotating > an emf is induced

    4. Operation

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    Operation of a DC Generator

    Driven by a source of mechanical power

    (prime mover)

    Prime mover

    A steam turbineA diesel engine

    An electric motor

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    Induced emf

    For a generator -> Generated emf

    For a motor -> Back emf

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    Developed Torque

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    Magnetization Characteristic

    If the armature is rotated at the rated speed;

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    Current in each conductor under a same pole mustbe in the same direction

    As the conductor moves from one pole to the next,

    there must be a reversal of the current

    This process of reversal is known as Commutation

    Commutation

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    Brush Positions

    GNA (Geometrical Neutral Axis)

    - axis of symmetry between 2 adjacent poles

    MNA (Magnetic Neutral Axis)- axis drawn perpendicular to the mean

    direction of the flux passing through the centre of

    the armature

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    For sparkles commutation, the brushes must lie

    along MNA

    With no current in the armature conductors, theMNA coincides with GNA.

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    Armature Reaction

    Flux by the field winding - main flux

    Flux by the armature winding - armature flux

    Armature flux distorts and weakens the main flux

    This action is called armature reaction

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    (Only one pole is shown for clarity)

    Effects: Flux weakening MNA shift (brushes are not aligned with MNA)

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    Solutions for Armature Reaction

    1) Brush shifting

    2) Commutating poles (Interpoles)

    3) Compensating winding

    Brush shifting

    Automatic brush shifting mechanisms (in largemachines)

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    Commutating poles (Interpoles)

    Small poles placed between the main poles Interpole winding - in series with armature

    winding Interpoles produce flux that opposes the

    armature fluxCompensating winding

    Slots cut in the pole faces Compensating winding on those slots Compensating winding produce flux that

    opposes the armature flux

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    1. Copper losses2. Rotational losses

    1. Friction & windage losses

    2. Magnetic loss (Core losses)

    3. Stray load losses

    Copper Losses

    Armature winding loss Field (shunt / series) winding loss

    Interpole winding loss (if any)

    Compensating winding loss (if any)

    5. Losses

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    Rotational Losses

    Friction and Windage Loss Bearing friction loss

    - friction between bearings and shaft

    Brush friction loss

    - friction between brushes and commutatorWindage loss

    - drag on the armature caused by air gap

    Magnetic Loss

    Hysteresis loss

    Eddy current loss

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    Stray Load Losses

    Due to the distorted flux due to armaturereaction

    About 1% of the output power in large

    machines Can be neglected in small machines

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    Power Flow Diagram For a Generator

    For a Motor

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    At starting Ea= 0

    As Rais very small, Iawill be extremely high

    This high current will permanently damage thearmature winding

    6. Starting a DC Motor

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    An external resistance is added in series with the

    armature circuit

    It is gradually decreased

    Finally, cut out from the armature circuit

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    7. Types of DC Motors

    1. Separately Excited DC Motor

    Field winding is supplied by a separate

    power source

    2. Series DC MotorField winding in series with armature

    winding

    3. Shunt DC Motor

    Field winding in parallel with armaturewinding

    4. Compound DC Motor

    2 field windings (series & shunt)

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    Separately Excited DC Motor

    External power source for field winding

    Mainly used in testing purposes (laboratories)

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    Series DC Motor

    Series filed winding carries rated Ia

    Ia changes with load -> main flux changes

    Flux is a function of Ia

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    High torque at low speeds

    Low torque at high speeds

    Suitable for hoists, cranes and electric trains

    Developed torque can be controlled bycontrolling the applied voltage

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    Example 1

    A series motor operates in the linear region inwhich the flux is proportional to the armaturecurrent. When the armature current is 12A, themotor speed is 600 rpm. The line voltage is 120 V,

    the armature resistance is 0.7 and the seriesfield winding resistance is 0.5.

    What is the torque developed by the motor?

    For the motor to operate at a speed of 2400 rpm,determine the;

    (a) armature current and

    (b) driving torque

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    For a constant Vs

    -> main flux is constant

    Shunt DC Motor

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    When the load (Ia) increases-> Eadecreases

    When armature reaction is negligibleFlux is constant speed decreases (curve a)

    When armature reaction is considered

    Flux decreases speed increases (curves b, c & d)

    Curve d is not desirable

    add stabilizing winding in series with armature

    winding

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    Compound DC MotorLongshunt compound DC motor:

    Shunt filed winding is connected across thepower source

    Flux created by the shunt filed winding is

    constant

    Shortshunt compound DC motor:

    Shunt field winding connected across the

    armature terminals

    Flux created is decreases with an increase in

    the load

    (due to voltage drop across series filed

    winding)

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    Long shunt compound DC motor

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    Short shunt compound DC motor

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    Cumulative compound motor:Flux produced by the series field windingaids the flux produced by the shunt fieldwinding

    Differential compound motor:Flux produced by the series field windingopposes the flux produced by the shunt

    filed winding

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    As we increase the load on a long-shuntcompound motor;

    1) Series winding current increases

    -> total flux increases/decreases

    (+) for cumulative and () for differential

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    2) Torque increases/decreases at a faster rate thana shunt motor

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    3) Increases the voltage drop across Ra and Rs

    - > decrease/increase the speed rapidly thanin a shunt motor

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    1. Armature resistance control method

    2. Field control method

    3. Armature voltage control method(Ward Leonard system)

    8. Speed Control

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    Add external resistance in the armature circuit

    Starting resistor can also be used

    Increase external resistance -> decrease speed

    Suitable to operate at a speed < rated speed

    (while delivering the same torque)

    Power loss in the external resistor

    Efficiency decreases

    Armature Resistance Control Method

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    Example 2

    A 220V DC shunt motor drives a pump whosetorque varies as the square of the speed. When themotor runs at 900 rpm, it takes 47A from the

    supply. The shunt filed current is 2A, and thearmature resistance is 0.5.

    What resistance must be inserted in the armature

    circuit in order to reduce its speed to 600 rpm?

    Calculate the power loss at the external resistance.

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    Control field current -> control flux

    Insert an external resistor

    in series with the shunt field winding

    in parallel with the series field winding

    Field current is very small -> power loss at theexternal resistor is small

    Flux decrease -> speed increase

    Suitable to operate at a speed > rated speed

    Filed Control Method

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    Inserting an external resistor in series with thearmature circuit

    = Applying a voltage < rated value across thearmature terminals

    Apply a reduced voltage across the armature

    terminals Voltage across the shunt field winding is held

    constant

    Armature Voltage Control Method(Ward Leonard System)

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    Requires 2 generators and an AC motor

    3 phase AC motor acts as a prime mover thatdrives both generators

    One generator (exciter) -> field winding

    Other generator -> provides a variable voltageacross armature terminals

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    Advantages:

    Eliminate the power loss exists in armatureresistance control method

    Wide and very sensitive speed control

    Disadvantages:

    Requires 2 power sources

    Expensive

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    References

    Electrical Machinery & Transformers

    Guru & Hizirogly

    Electrical Machines Theory & Practice

    M N Bandyopadhyay

    Electrical Machinery Fundamentals

    Stephan J Chapman