3-phase induction machines

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    Lecture 24 - EE743Lecture 24 - EE743

    3-Phase Induction Machines

    Torque Speed characteristics

    Professor: Ali KeyhaniProfessor: Ali Keyhani

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    Importance of T-speed characteristics

    s Torque speed characteristic of a motor is important from

    the point of view of its applications to specific situations.

    To calculate the torque produced by the machine, first, we

    compute the motor power. The motor power, or the

    mechanical power supplied to the load is

    The electrical power inputted to the machine can be

    calculated from the eq. circuit given below

    lossesinem PPP =

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    Importance of T-speed characteristics

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    Machine Torque

    s Power dissipated is

    s Motor power Pem is

    s Motor torque can be calculated from

    { }

    +==s

    RRIIVP

    '2

    1

    2

    1*

    111 3~~

    Re3

    extrotor RRR

    XaX

    RaR

    +==

    =

    2

    22'

    2

    22'

    2

    ( ) ( )'212

    1221

    2

    1 33 RRIRaRIP +=+=

    ( ) 21'2

    '21

    '2

    1

    2

    1

    133 IR

    s

    sRR

    s

    RRIPem

    =

    +

    +=

    memem TP =2

    1'2

    13IR

    s

    sT

    m

    em

    =

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    Machine Torque

    s Since Tm can be written as

    s Substituting for I1 in equation (3), we will have

    ( )ssyncm = 1

    2

    1

    '23 I

    s

    RT

    sync

    em

    =

    ( )

    2'

    21

    2'2

    1

    2

    12

    1

    XXs

    RR

    VI

    ++

    +

    =

    ( )2'212'

    21

    2

    1

    '

    23

    XXs

    RR

    Vs

    RTsync

    em

    ++

    +=

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    Power calculations

    s Figure 2 shows the plot of equation (3) for the values of slip

    from zero to unity. In Fig.1 . This

    corresponds to the normal range of the speed of an induction

    motor from starting (m=0, s=1) to the synchronous speed (m=

    sync, s=0)

    ( )extRRaR += 22'

    2

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    smax and Tmax calculation

    s To find smax first set derivative of (4) with respect to s

    equal to zero.

    s Which will results in

    s substituting smax in (4) will result in Tmax

    0=ds

    dTm

    ( )2'2121

    '2

    max

    XXR

    Rs

    ++=

    ( )

    +++

    =2'

    21211

    2

    max2

    3

    XXRR

    VT

    sync

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    Torque-speed characteristic

    s Equation (5) shows that the slip at which the maximum torque

    occurs is proportional to the rotor resistance. Equation (6) shows

    that the maximum torque is independent of the rotor resistance

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    Torque-speed characteristic

    s Case 1: sync and m are rotating in the same direction and

    sync is rotating faster than m.

    s Case 2: sync and m are rotating in the same direction and sync is rotating slower than m.

    s Case 3: sync and m are rotating in different directions.

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    Torque-speed characteristic. Case 1.

    s Case 1: sync and m are rotating in the same direction and

    sync is rotating faster than m. This case is the normal operation of the induction machine. Machine

    operates as a motor. Note also in equation (7) sync and m are inthe same direction and the slip is positive for motor operation

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    Torque-speed characteristic. Case 2.

    s Case 2: sync and m are rotating in the same direction and

    sync is rotating slower than m. If the speed of the machine is increased beyond its synchronous

    speed by an external prime motor, but still rotated in the same

    direction as the stator field, the slip will be negative (s

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    Torque-speed characteristic. Case 3.

    s Case 3: sync and m are rotating in different directions. Suppose an induction motor is operating under normal conditions at

    the same value of positive slip in stable region (0

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    Example 1

    s On no-load a 3-phase delta-connected induction motor

    takes 6.8A and 390W at 220V line to line. R1=0.1/phase,friction and windage losses are 120W. Determine Xm,and

    Rm

    of the motor equivalent circuit.

    AII linephase 926.33

    8.6

    3===

    LLphase VVV == 220 WRI phasephase 54.12 =

    m

    phase

    RVWlossesCore

    2

    46.8854.13120390 ===

    == 14.54746.88

    2202

    mR ==

    110828.1

    1 3

    m

    mR

    G

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    Example 1

    === 11084.17

    220

    926.3 3

    V

    IY mm

    === 1

    10746.17

    1 322mm

    mm GYXB = 35.56mX

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    Example 2

    s The motor of the previous example take 30A and 480W at

    36V line-to-line, when the rotor is blocked. Determine the

    complete equivalent circuit of the motor. Assume that

    X1=X2.

    ( ) eqeqeq XRZXX ==

    ==+ 0.2533.0

    3/30

    36 22

    22'21

    ( )( )

    eqRRR ===+ 533.03/30

    3/4802

    '21

    == 433.01.0 '21 RsoR

    == 12

    21eqX

    XX

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    Example 3

    s An induction motor has an output of 30kW at =0.86. Forthis operating condition Pcoil,1=Pcoil,2=Pcore=Prot.Determine the slip

    3,

    0

    inP

    PEff=

    WEff

    PPin 884,34

    86.0

    000,3003, ===

    WPloss 884,4000,30884,343, ==

    M

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    Example 3

    WPPPPP rotcoreRAG 663,33'20=+++=

    3,

    3,'2

    AG

    R

    P

    Ps = WP

    R221,1

    4884,4

    '2

    ==

    %6.3036.0663,33

    221,1ors ==

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    Example 4

    s A wound rotor six-pole 60Hz ind. motor has R2=0.8 andruns at 1152 rpm (s=0.04) at a given load. The load torque

    remains constant at all speeds. How much resistance must

    be inserted in the rotor circuit to change the speed to 960

    rpm (s=0.2). Neglect the motor leakage reactance, X1 and

    X2.

    The air gap power function is:

    ( )2'212'

    21

    21

    '2

    '2

    2'2 33

    XXs

    RR

    V

    s

    R

    s

    RIPg

    ++

    +

    =

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    Example 4

    s If (see eq. circuit ), the voltage, current,

    air-gap power, and torque conditions remain the same, i.e

    tconssR tan

    '2 =

    ..

    '

    2 ConstTthenConstsR ==

    2.004.0

    ''2

    '2 insertRRR +=

    === 2.38.0)8.0(504.0

    2.0 '2

    '2

    ' RRRinsert

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    Example 5

    s A 400V, 3-phase WYE connected motor has

    , and

    using the approx. eq. circuit. Determine the max.

    electromagnetic power, Pd

    ( ) phasejZ /2.16.01 += ( ) phasejZ /3.15.0'2 +=

    ( )2'212'

    21

    1

    21

    1'2

    XXs

    RR

    V

    ZZ

    VI

    ++

    +

    =+

    = VV 2313

    4001 ==

    ( ) 22

    '2

    5.25.0

    6.0

    231

    +

    +

    =

    s

    I

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    Example 5

    ( ) ( )sfunctionIRs

    sPsRIPP ggd =

    ===2'

    2'2

    '2

    2'2

    11

    CBss

    ssAPd

    ++

    =2

    2

    ( )

    ( )( )Bs

    CBss

    ssA

    CBss

    sA

    ds

    dPd +++

    ++

    == 221022

    2

    2155.0

    max=

    dPats

    ( )( )

    WCBss

    ssAP

    s

    phased 962,6

    155.0

    22

    2

    max,, =++

    ==

    WP phased 886,20962,633max,, ==