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    1

    Induction Motor

    (Asynchronous Motor)

    ELECTRICAL MACHINES

    Compiled by

    Prof Mitali Ray

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    2

    Learning Outcomes

    At the end of the lecture, student should to:

    Understand the principle and the nature of 3 phase

    induction machines.

    Perform an analysis on induction machines which is

    the most rugged and the most widely used machine

    in industry.

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    3

    Contents

    Overview of Three-Phase Induction Motor

    Construction

    Principle of Operation

    Equivalent Circuit

    Power Flow, Losses and Efficiency

    Torque-Speed Characteristics

    Speed Control

    Overview of Single-Phase Induction Motor

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    4

    Overview of Three-Phase Induction

    Motor

    Induction motors are used worldwide in many

    residential, commercial, industrial, and utility

    applications.

    Induction Motors transform electrical energy intomechanical energy.

    It can be part of a pump or fan, or connected to some

    other form of mechanical equipment such as a winder,

    conveyor, or mixer.

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    5

    Introduction

    General aspects

    A induction machine can be used as either a induction

    generator or a induction motor.

    Induction motors are popularly used in the industry Focus on three-phase induction motor

    Main features: cheap and low maintenance

    Main disadvantages: speed control is not easy

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    Construction

    The three basic parts of an AC motor are the rotor, stator,and enclosure.

    The stator and the rotor are electrical circuits that perform aselectromagnets.

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    Squirrel Cage Rotor

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    MZSFKEE, UMP

    9

    Construction (Stator construction)

    The stator is the stationary electrical part of the motor.

    The stator core of a National Electrical Manufacturers Association(NEMA) motor is made up ofseveral hundred thin laminations.

    Stator laminations are stacked togetherforming a hollow cylinder.Coils of insulated wire are inserted into slots of the stator core.

    Electromagnetism is the principle behind motor operation. Each

    grouping of coils, together with the steel core it surrounds, form anelectromagnet. The stator windings are connected directly to thepower source.

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    Construction (Rotor construction)

    The rotor is the rotating part of the electromagnetic

    circuit.

    It can be found in two types:

    Squirrel cage

    Wound rotor

    However, the most common type of rotor is the

    squirrel cage rotor.

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    Induction motor types:

    Squirrel cage type:

    Rotor winding is composed of copper bars embedded in

    the rotor slots and shorted at both end by end ringsSimple, low cost, robust, low maintenance

    Wound rotor type:

    Rotor winding is wound by wires. The winding terminalscan be connected to external circuits through slip ringsand brushes.

    Easy to control speed, more expensive.

    Construction (Rotor construction)

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    MZSFKEE, UMP

    12

    Construction (Rotor construction)

    Wound Rotor

    Squirrel-Cage Rotor

    /rotor winding

    Short circuits all

    rotor bars.

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    13

    Construction (Enclosure)

    The enclosure consists of a frame (or yoke) and two endbrackets (or bearing housings). The stator is mountedinside the frame. The rotor fits inside the stator with aslight air gap separating it from the stator. There is NOdirect physical connection between the rotor and thestator.

    Stator

    Rotor

    Air gap

    The enclosure also protects the electricaland operating parts of the motor from

    harmful effects of the environment in whichthe motor operates. Bearings, mounted onthe shaft, support the rotor and allow it toturn. A fan, also mounted on the shaft, isused on the motor shown below for cooling.

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    Construction (Enclosure)

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    Nameplate

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    Rotating Magnetic Field

    When a 3 phase statorwinding is connected to a 3 phasevoltage supply, 3 phase current will flow in the windings,which also will induced3 phase flux in the stator.

    These flux will rotate at a speed called a SynchronousSpeed, n

    s

    . The flux is called as Rotating magnetic Field

    Synchronous speed: speed of rotating flux

    Where; p = is the number of poles, and

    f = the frequency of supply

    p

    fns

    120

    RMF

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    a Fc

    -93

    10

    113

    216

    -1.5

    -1

    -0.5

    0

    0.5

    1

    1.5

    a

    cb

    b c

    a

    a

    c

    b

    b c

    a

    a

    c b

    b c

    a

    a

    c b

    b c

    Fb

    Fa F

    FbFc

    F

    Fa

    F

    Fb

    Fc Fc Fb

    F

    Space angle () in degrees

    FFa Fc

    Fb

    t = t0= t4

    t = t1t = t2 t = t3

    t = t0= t4

    RMF(Rotating Magnetic Field)

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    AC Machine Stator

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    Axis of phase a

    a

    a

    -90 -40 10 60 110 160 210 260-1

    -0.8

    -0.6

    -0.4

    -0.2

    0

    0.2

    0.4

    0.6

    0.8

    1

    Fa

    Space angle (theta) in degrees

    t0

    t01

    t12

    t2

    a

    MMF Due to a phase current

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    1 Cycle

    Amp

    timet0

    t1 t2 t3 t4

    t01 t12Currents in different phases of AC Machine

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    Slip Ring Rotor

    The rotor contains windings similar to stator.

    The connections from rotor are brought out using slip rings that

    are rotating with the rotor and carbon brushes that are static.

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    MZSFKEE, UMP 22

    Slip and Rotor Speed

    1. Slip s

    The rotor speed of an Induction machine is different from thespeed of Rotating magnetic field. The % difference of the speed

    is called slip.

    Where; ns = synchronous speed (rpm)

    nr= mechanical speed of rotor (rpm)

    under normal operating conditions, s= 0.01 ~ 0.05, which is

    very small and the actual speed is very close to synchronous

    speed.

    Note that : s is not negligible

    )1( snnOR

    n

    nns sr

    s

    rs

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    23

    Slip and Rotor Speed

    Rotor Speed

    When the rotor move at rotor speed, nr (rps), the stator flux will

    circulate the rotor conductor at a speed of (ns-nr) per second.

    Hence, the frequency of the rotor is written as:

    Where; s= slip

    f = supply frequency

    sf

    pnnf rsr

    )(

    fsfiii

    iipnn

    f

    nnRotorAt

    ipn

    f

    nstatorAt

    Note

    r

    rsr

    p

    f

    rs

    s

    p

    f

    s

    .:)()(

    ).....(120

    )(

    :

    ).....(120

    :

    :

    120

    120

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    24

    Principle of Operation

    Torque producing mechanismWhen a 3 phase stator winding is connected to a 3

    phase voltage supply, 3 phase current will flow in thewindings, hence the stator is energized.

    A rotating flux is produced in the air gap. The flux induces a voltage Ea in the rotor winding (like atransformer).

    The induced voltage produces rotor current, if rotor

    circuit is closed.The rotor current interacts with the flux , producing

    torque. The rotor rotates in the direction of the rotatingflux.

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    Direction of Rotor Rotates

    Q: How to change the direction of

    rotation?

    A: Change the phase sequence of the

    power supply.

    E i l t Ci it f I d ti

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    26

    Conventional equivalent circuit

    Note:

    Never use three-phase equivalent circuit. Always use per-

    phase equivalent circuit. The equivalent circuitalways bases on the Y connection

    regardless of the actual connection of the motor.

    Induction machine equivalent circuit is very similar to the

    single-phase equivalent circuit of transformer. It is

    composed of stator circuit and rotor circuit

    Equivalent Circuit of Induction

    Machines

    E i l t Ci it f I d ti

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    Step1 Rotor winding is open(The rotor will not rotate)

    Note: the frequency ofE2 is the same as that ofE1 since the rotor is at

    standstill. At standstill s=1.

    Equivalent Circuit of Induction

    Machines

    f f

    E i l t Ci it f I d ti

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    Equivalent Circuit of Induction

    Machines

    E i l t Ci it f I d ti

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    Equivalent Circuit of Induction

    Machines

    Step2 Rotor winding is shorted

    (Under normal operating conditions, the rotor winding is shorted. The slip is s)

    Note:

    the frequency ofE2 isfr=sfbecause rotor is rotating.

    f fr

    E i l t Ci it f I d ti

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    Step3 Eliminatef2

    Keep the rotor current same:

    Equivalent Circuit of Induction

    Machines

    E i l t Ci it f I d ti

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    MZSFKEE, UMP

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    Step 4 Referred to the stator side

    Note: X2 and R2 will be given or measured. In practice, we do not

    have to calculate them from above equations.

    Always refer the rotor side parameters to stator side.

    Rcrepresents core loss, which is the core loss of stator side.

    Equivalent Circuit of Induction

    Machines

    E i l t Ci it f I d ti

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    IEEE recommended equivalent circuit

    Note: Rc is omitted. The core loss is lumped with the

    rotational loss.

    Equivalent Circuit of Induction

    Machines

    Equivalent Circuit of Induction

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    IEEE recommended equivalent circuit

    Note: can be separated into 2 PARTS

    Purpose :

    to obtain the developed mechanical

    Equivalent Circuit of Induction

    Machines

    I1 1R1X

    mX

    '

    2X'2R

    s

    sR

    1'21V

    s

    R2

    ssRR

    sR )1(2

    22

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    34

    Analysis of Induction Machines

    For simplicity, let assume

    Is=I1 , IR=I2

    (s=stator, R=rotor)

    RmsTotal

    sss

    cmm

    cmcm

    RR

    R

    ZZZZ

    jXRZ

    neglectedRjXZ

    neglectedRjXRZ

    jXsRZ

    //

    ;

    ;

    ;//

    ;''

    ZRZm

    Zs

    Vs1

    Is1 Im1 IR1

    T

    s

    sZ

    V

    I

    1

    1

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    Analysis of Induction Machines

    m

    RM

    m

    R

    RM

    R

    s

    T

    mRRM

    Z

    VI

    Z

    VIHence

    VZ

    ZZV

    RulesDiv idingVoltage

    1

    1

    1

    1

    11

    ,

    //

    ,

    ZRZm

    Zs

    Vs1

    Is1 Im1 IR1

    11

    11

    ,

    s

    Rm

    mR

    s

    Rm

    Rm

    I

    ZZ

    ZI

    IZZ

    ZI

    RulesDividingCurrent

    OR

    Note : 1hp =746Watt

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    Power Flow Diagram

    Pin (Motor)

    Pin (Stator)

    Pcore loss(Pc)

    Pair Gap

    (Pag)

    PdevelopedPmechanical

    Pconverted

    (Pm)

    Pout, Po

    Pstator copper

    loss, (Pscu)

    Protor copper

    loss (Prcu)Pwindage, friction,

    etc

    (P - Given)

    cos3 ssIV

    s

    RI RR

    ''32

    2

    3

    c

    RM

    R

    V ''32

    RR RI

    s

    sRI RR

    1''3

    2

    Whp 7461

    ss RI2

    3

    Pin (Rotor)

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    Power Flow Diagram

    Ratio:

    Pag Prcu Pm

    s

    RI RR

    ''3 2 ''3 2 RR RI

    s

    sRI RR

    1''3 2

    s1 11

    s1

    1 s s1

    Ratio makes the analysis simpler to find the value of the particular power if we haveanother particular power. For example:

    s

    s

    P

    P

    m

    rcu

    1

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    Efficiency

    WattxWhpxPIVP

    otherwise

    PPPPPP

    givenarePif

    PP

    out

    ssin

    mo

    lossesino

    losses

    in

    out

    746746cos3

    ,

    ,

    %100

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    39

    Torque-Equation

    Torque, can be derived from power equation in term ofmechanical power or electrical power.

    nPTHence

    sradn

    whereTPPower

    260,

    )/(60

    2,,

    r

    oo

    r

    m

    m

    n

    PTTorqueOutput

    n

    PTTorqueMechanical

    Thus

    2

    60,

    2

    60,

    ,

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    Torque-Equation

    Note that, Mechanical torque can written in terms of circuit

    parameters. This is determined by using approximationmethod

    .. .

    .. .

    .. .

    )1('

    '3

    )1('

    '3

    2

    2

    r

    RR

    r

    mm

    mrmR

    Rm

    s

    s

    RI

    PT

    TPandss

    RIP

    22

    2

    )'()'(

    '

    2

    )(3

    RR

    R

    s

    RM

    msXR

    sR

    n

    VT

    Hence, Plot Tmvs s

    Tm

    ns

    smax is the slip for Tmax to occur

    s=1

    Tst

    Tmax

    smax

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    Torque-Equation

    22

    2

    )'()'(

    '

    602

    )(3

    1,

    RsRs

    R

    s

    s

    stXXRR

    R

    n

    VT

    sTorqueStarting

    22

    2

    max

    22max

    )'()(

    1

    6022

    )(3

    )'()('

    Rssss

    s

    Rs

    R

    XXRRnVT

    XRRs

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    Speed Control

    There are 3 types of speed control of 3 phaseinduction machines

    i. Varying rotor resistance

    ii. Varying supply voltage

    iii. Varying supply voltage and supply frequency

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    Varying rotor resistance

    Forwound rotor only Speed is decreasing

    Constant maximum

    torque

    The speedat which maxtorque occurs changes

    Disadvantages:

    large speed regulation

    Power loss in Rext reduce the efficiency

    T

    ns~nNL

    T

    nr1nr2nr3 n

    nr1< nr2< nr3R1R2R3

    R1

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    Varying supply voltage

    Maximum torque changes

    The speed which at max

    torque occurs is constant

    (at max torque, XR=RR/s

    Relatively simple methoduses power electronics

    circuit for voltage controller

    Suitable for fan type load

    Disadvantages : Large speed regulation since

    ~ ns

    T

    ns~nNL

    T

    nr1nr2nr3n

    nr1> nr2 > nr3

    V1

    V2

    V3

    V1

    >V2

    >V3

    V

    decreasing

    Varying supply voltage and supply

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    The best method since

    supply voltage and supply

    frequency is varied to keepV

    /f constant Maintain speed regulation

    uses power electronics

    circuit for frequency andvoltage controller

    Constant maximum torque

    Varying supply voltage and supply

    frequency

    T

    nNL1

    T

    nr1nr2nr3 n

    f

    decreasing

    nNL2nNL3