Chapter 4 Ee 342 Ac Fundamentals

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    Chapter 4 (P#230)

    AC MachineryFundamentals

    Pole

    DC excitation

    windingFan

    Slip

    rings

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    AC Generator (Field Fix Armature Rotating)

    Will it work asAC Generatorif theArmature is

    fixed and Field is rotating ?

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    4.1 A simple Loop in a uniform Magnetic Field (230)

    (Voltage Induced in a simple rotating Loop (Page 231 ))

    eind = ZBVLsin single conductor (Z=1)

    eind = 2 BVLsin loop (2 conductors Z=2)

    eind = maxsin t [4-11 ]Z

    S

    The voltage generated in the loop is a sinusoidal whose

    magnitude is equal to the product of the flux inside the machine

    and the speed rotating of the machine

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    4.1 A simple Loop in a uniform Magnetic Field (230)

    (Torque Induced in a current-carrying Loop (Page 234 ))

    F = ZBILsin single conductor (Z=1)

    F = 2 BILsin loop (2 conductors Z=2)

    ind = k Bloopx BS [4-20 ]

    The torque induced in the loop is proportional to the strength of

    the loops magnetic field, the strength of the external magnetic

    field, and the sine of the angle between them.

    r

    N

    S

    F

    F

    X

    X

    Bloop

    BS

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    4.2 (page 238) Rotating Magnetic Field

    (Page 242 - The relationship between Electric Frequency and the

    speed of Magnetic Field Rotation)

    ).(Pn

    f me

    344

    120

    nm = speed of magnetic field in rev/min

    fe = electric frequency in Hz (Hertz cycle/sec)

    P = Number of poles (North south are counted as 2-poles)

    How the stator magnetic field be made to rotate?

    The fundamental principle of ac machine operation is that:

    IF a 3-phase set of currents, each of equal magnitude and

    differing in phase by 1200, flows in a 3-phase winding, then it willproduce a rotating magnetic field of constant magnitude (1.5

    times the peak value).

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    The three phase winding consists of three separate windings

    spaced 1200 electrical apart around the surface of the machine

    (Page 244)Reversing the Direction of Magnetic Field Rotation

    If the current in any two of the three coils is swapped, the direction

    of magnetic fields rotation will be reversed. This means that it is

    possible to reverse the direction of rotation of an ac motor just byswitching the connections on any two of three coils.

    http://en.wikipedia.org/wiki/File:3-phase_flow.gif
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    Page 241 Proof of the Rotating Magnetic Field

    Next Few Slides Will Demonstrate The

    Revolving Magnetic Field in The Stator Windings

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    ALTERNATOR (AC Generator or Synchronous Generators)

    The elementary 3-phase 2-pole synchronous generator has a

    stator equipped with 3 coils displaced 120o from each other;

    although shown as concentrated, they actually are distributed.

    When the rotor is excited with dc and rotated, the resultant

    field will also rotate so that sinusoidal voltages are generated

    in the 3 stator phases, displaced 120o in time and having a

    frequency directly related to rotor speed.

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    Page 241 Proof of the Rotating Magnetic Field

    A -C B -A C

    0o 360o

    -C

    -B

    CB

    A

    -A

    -B

    Stator winding

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    Phase A

    magnetic axis

    corresponding coil

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    Phase Bmagnetic axis

    corresponding coil

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    Phase C

    magnetic axis

    corresponding coil

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    in

    out

    P

    P)(Efficiency

    in

    lossesin

    P

    PP

    lossesout

    out

    PP

    P

    in

    losses

    P

    P 1

    1. Electrical Losses or Copper Losses (I2R)

    2. Core Losses=Hysteresis+Eddy Current Losses (Proportional to Speed & )

    3. Mechanical Losses (Proportional to speed)

    4. Stray Load Losses 1% of the Full Load rated Capacity (100 W 1 W)

    Armature (Stator) Losses Field (Rotor) Losses ( Fixed IF )

    AAA RIPlossArmature23 FFF RIP)Rotor(lossField

    2

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    Pout=VIAcos=3VLILcos

    Stray

    Losses

    1% of Rating

    Mechanical

    Losses

    = Friction

    + WindageLosses

    Core

    Losses

    = EddyCurrent

    + HystersisLosses

    I2R Losses= Armature

    + Field

    Losses

    Mechanical

    in= appm

    Pout = Pin - Losses

    indm

    Pconv

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    StrayLosses

    1% of Rating

    Mechanical

    Losses

    = Friction

    + Windage

    Losses

    Core

    Losses

    = EddyCurrent

    + Hystersis

    Losses

    I2R Losses

    = Armature

    + FieldLosses

    Pout=VIAcos=3 VLILcos

    Pout = Pin - Losses

    indm

    Pconv

    Mechanical

    Pout= indm

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    AC Generator are compared by their

    VOLTAGE

    POWER RATINGS

    EFFCIENCIES

    VOLTAGE REGULATIONS

    AC Motors are compared by their:

    SPEED

    POWER RATINGS

    EFFCIENCIES

    SPEED REGULATIONS

    FL

    FLNLgulationReSpeed

    FL

    FLNL

    V

    VVgulationReVoltage

    Assume the Motors are run

    from a constant source

    (VT), unless voltage change

    is specified

    Assume the Generators are are

    run from a constant Speed

    source called Prime Mover,

    unless speed change is specified

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    END OF CHAPTER 4

    NEXT CHAPTER 5

    Synchronous Generators

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    http://www.ece.umn.edu/users/riaz/animations/spacevectors.html

    http://www.coolmagnetman.com/magacmot.htm

    M t G t

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    Motor Generator

    RA

    EA

    RA

    EA

    IA= IL

    +

    -

    +

    -

    +

    -

    +

    -

    IF

    VTRA

    EA

    RA

    EA

    IA= IL

    +

    -

    +

    -

    IF

    LVT

    Separately

    &

    shunt

    M/R & G/R

    )R+R(IE=V SAAAT

    RA

    EA

    RA

    EA

    +

    -

    +

    -

    IA= IL=IF

    VTVT

    RA

    EA

    RA

    EA

    IA= IL=IF

    RL

    2

    AI'K=

    EA=K

    VT=EAIARA

    EA=K

    T=KIA

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    RA

    EA

    RA

    EA

    RA

    EA

    RA

    EA

    RA

    EA

    RA

    +-

    +

    -

    +

    -

    RA

    EA

    RA

    EA

    RA

    EA

    IA= IL

    +

    -

    +

    -

    +

    -

    +

    -

    IF

    T

    IAIL

    http://en.wikipedia.org/wiki/File:3-phase_flow.gif