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Lecture 24 Lecture 24 - - EE743 EE743 Induction Machines Torque Speed characteristics

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  • Lecture 24 Lecture 24 -- EE743EE743

    Induction MachinesTorque Speed characteristics

  • 2

    Importance of T-speed characteristics

    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 =

  • 3

    Importance of T-speed characteristics

  • 4

    Machine Torque

    Power dissipated is

    Motor power Pem is

    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

    122

    1

    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

    =

  • 5

    Machine Torque

    Since Tm can be written as

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

    ( )ssyncm = 1

    2

    1

    '23 I

    s

    RT

    sync

    em

    =

    ( )2'212'

    21

    2

    12

    1

    XXs

    RR

    VI

    ++

    +

    =

    ( )2'212'

    21

    2

    1'23

    XXs

    RR

    V

    s

    RT

    sync

    em

    ++

    +

    =

  • 6

    Power calculations

    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

  • 7

    smax and Tmax calculation

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

    equal to zero.

    Which will results in

    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

  • 8

    Torque-speed characteristic

    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

  • 9

    Torque-speed characteristic

    The machine is operating as a motor for the range of s for

    which the torque-speed curves are shown in fig.1 and fig.2.

    In this range, torque is positive and sync is greater than

    rotor speed m. Note that the torque is zero at slip equal to

    zero. As was state before, slip is given by

    Let us consider three different cases:

    sync

    msyncs

    =

  • 10

    Torque-speed characteristic

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

    sync is rotating faster than m.

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

    sync is rotating slower than m.

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

  • 11

    Torque-speed characteristic. Case 1.

    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 in

    the same direction and the slip is positive for motor operation

  • 12

    Torque-speed characteristic. Case 2.

    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

  • 13

    Torque-speed characteristic. Case 3.

    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

  • 14

    Example 1

    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.

    AI

    I linephase 926.33

    8.6

    3===

    LLphase VVV == 220 WRI phasephase 54.12 =

    m

    phase

    R

    VWlossesCore

    2

    46.8854.13

    120390==

    =

    == 14.54746.88

    2202

    mR ==

    110828.1

    1 3

    m

    mR

    G

  • 15

    Example 1

    ===

    11084.17

    220

    926.3 3

    V

    IY mm

    ===

    110746.17

    1 322mm

    m

    m GYX

    B = 35.56mX

  • 16

    Example 2

    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

    21

    eqXXX

  • 17

    Example 3

    An induction motor has an output of 30kW at =0.86. For

    this 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

  • 18

    Example 3

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

    3,

    3,'2

    AG

    R

    P

    Ps = WP

    R221,1

    4

    884,4'2

    ==

    %6.3036.0663,33

    221,1ors ==

  • 19

    Example 4

    A wound rotor six-pole 60Hz ind. motor has R2=0.8 and

    runs 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

    ++

    +

    =

  • 20

    Example 4

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

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

    tconss

    Rtan

    '2 =

    ..'2 ConstTthenConst

    s

    R==

    2.004.0

    ''2

    '2 insertRRR +=

    === 2.38.0)8.0(504.0

    2.0 '2

    '2

    'RRRinsert

  • 21

    Example 5

    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

  • 22

    Example 5

    ( ) ( )sfunctionIRs

    sPsRIPP ggd =

    ===

    2'2

    '2

    '2

    2'2

    11

    ( )CBss

    ssAPd

    ++

    =

    2

    2

    ( ) ( )( )

    ( )BsCBss

    ssA

    CBss

    sA

    ds

    dPd +++

    ++

    == 2

    210

    22

    2

    2155.0

    max=

    dPats

    ( )( )

    WCBss

    ssAP

    s

    phased 962,6

    155.0

    22

    2

    max,, =++

    =

    =

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