Module 8 Three Phase Systems v3

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    Three-Phase Systems

    EE 102 Circuits 2

    Module 8

    by:Cesar G. Manalo !r.

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    Objectives

    Defne a three-phase system.

    Describe the wye and delta-type connections in three-phase systems.Solve voltages and currents in three-phase system.Describe a single-phase three-wire system.

    Solve voltages and current in single-phase three-wiresystem.

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    Introduction

    The three-phase (3-φ) ! generators (alternators) has

    3 sets o" armature windings called phase windings .#ach o" the 3 windings develop e$actly the samesinusoidal voltages (same magnitude and "re%uency)called phase voltage but are &' electrical degrees

    apart.

    N S

    &' edeg

    &' edeg

    3-phase 2-pole alternator

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    Introduction

    n most cases* the winding that produces the +u$ is

    the one revolving and the armature winding (thatdevelops phase voltages) is stationary.

    The 3 sets o" windings can be wired together to "ormeither a delta(,) connection or a wye( ) connection.

    a

    c

    b

    a

    c b

    E aa’

    E cc’

    E bb’

    c

    c

    bb

    a

    a

    N S

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    Introduction

    Y-connected alternator

    a

    c

    ba

    c b

    E aa’

    E cc’

    E bb’ N S

    c

    cbb

    a

    a

    a

    b

    c

    a

    b

    c

    3-phase 2-pole Y-connected alternat

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    Introduction

    Y-connected alternator

    a

    c

    ba

    c b

    E aa’

    E cc’

    E bb’

    a

    b

    c

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    Introduction

    Y-connected alternator

    a

    c

    ba

    c b

    E aa’

    E cc’

    E bb’

    /

    !

    a

    c

    b

    E a

    E c E b

    /

    !

    n

    Y-connected alternator withcommon point called neutral (n)

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    Line-to-line olta!e in 3-"hase Y-connected #lternators

    n a balanced system*each o" the threeinstantaneous voltagesa *b * 0 c have e%ualamplitudes but areseparated "rom the other

    voltages by a phaseangle o" &' o.

    $ #N

    $ %N

    $ &N

    '2 o

    '2 o

    '2 o

    $ #N

    $ %N$ &N

    #

    %

    &

    $ #%

    $ %&

    $ N

    3-phase alternator with the phases replaced3 sin!le-phase alternators* e-connected 3-phase alternator

    "hasor dia!ramo+ phase volta!

    a

    c

    b

    E a

    E c E

    b

    /

    !

    1

    2

    2 2

    -

    - -

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    Line-to-line olta!e in 3-"hase Y-connected #lternators

    $ #N

    $ %N

    $ &N

    '2 o

    '2 o'2 o

    )( BN AN NB AN AB E E E E E −+=+=

    -$ %N

    a

    bc

    #

    %

    &

    $ #%

    $ %&

    $ N

    $ #N

    $ N%, o

    where $ #N is the phase voltage o" alternator a

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    Line-to-line olta!e in 3-"hase Y-connected #lternators

    $ #N

    )( BN AN NB AN AB E E E E E −+=+=

    -$ %N # /

    3 # 1 2

    ( - # / 1 )

    AN AN AB E E E 73.13 == BN BN BC E E E 73.13 ==CN CN CA E E E 73.13 ==

    a

    bc

    #

    %

    &

    $ #%

    $ %&

    $ N

    $ #N

    $ N%

    , o3 o

    here+ore. the line-to-line volta!es o+ a w e-connected alternator is '/03 times its phase volta!e/

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    Line-to-line olta!e in 3-"hase Y-connected #lternators

    a

    bc

    #

    %

    &

    $ #%

    $ %&

    $ N

    $ #N

    $ %N

    $ &N

    '2 o

    '2 o

    '2 o

    $ #%$ '2 o

    '2 o '2 o

    here+ore. the line-to-line volta!es o+ a w e-connected alternator is '/03 times its phase volta!e.and the are '2 o out o+ phase +rom each other/

    $ %&

    "hasordia!ram o+phase and linevolta!es o+ a 3-phase Y-connectedalternator

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    Line-to-line olta!e in 3-"hase Y-connected #lternators

    #&O1 "1

    • The line-to-line voltage o" a 3-phase alternator is '3 4 asmeasured by an ! voltmeter. 5hat is the phase voltage i"measured by the same voltmeter i" the alternator isconnected in wye 6 5rite the polar "orm o" all line-to-line andphase voltages.

    Illustrative "roblem ''

    Solution78et7 # / line-to-line voltage between 0 /

    # 1 phase voltage o" phase 1.

    V E E

    E E

    AB AN

    AN AB

    9.13273.1

    23073.1

    73.1

    ===

    =

    V E

    V E

    V E

    V E V E

    referenceV E

    CA

    BC

    AB

    CN

    BN

    AN

    °∠=°−∠=

    °∠=°∠=

    °−∠=

    °∠=

    150230

    90230

    30230

    1209.1321209.132

    )(09.132

    $ #N

    $ %N

    $ &N

    '2 o

    '2 o'2 o

    $ #%

    '2 o

    '2 o '2 o

    $ %&

    $

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    Line &urrent in 3-"hase Y-connected#lternators

    a

    bc

    #

    %

    &

    #%

    %&

    N I

    a

    I b

    I c

    ' 2 ( o

    ' 2 ( o

    ' 2 ( o

    I#

    I%

    I&

    Ia

    IbIc I #

    I &

    I % "hase and linecurrent phasordia!ram o+ abalanced-loaded 3-phase alternator

    • he current on a line is e ual to the currentthrou!h the phase to which that line isconnected/ hat is. I # I a . I % I b . I & I c /

    • *hen the e4ternal load on a 3-phasealternator is 5balanced6. the line and phasecurrents are all '2 o out o+ phase +rom each

    # 1

    # /1

    # !1

    #lternator

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    Line-to-line olta!e in 3-"hase 7-connected #lternators

    • n a ,-connected 3-phase alternator* there is no

    neutral pt.• The phase windings are connected one a"ter the

    other "orming a delta or closed loop.• The line-to-line voltages e%uals the phase voltages

    both in magnitude and in direction because thephases are connected directly to the lines.

    $ #

    $ %

    $ &'2 o

    '2 o

    '2 o$ #

    $ %

    $ &

    #

    %

    &

    $ #%

    $ %&

    $

    7-connected 3-phase alternators "hasor dia!ram

    2

    2

    2

    -

    -

    -

    $ #%

    $ %&

    $

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    Line-to-line &urrent in 3-"hase 7-connected #lternators

    $ #

    $ %

    $ &'2 o

    '2 o

    '2 o$ #

    $ %

    $ &

    #

    %

    &

    $ #%

    $ %&

    $

    7-connected 3-phase alternators "hasor dia!ram

    2

    2

    2

    -

    -

    -

    $ #%

    $ %&

    $

    C CA

    B BC

    A AB

    E E E E

    E E

    ==

    =

    I#%

    I%&I

    I#%

    I%&

    I&#

    CACA BC C

    BC BC AB B

    AB ABCA A

    I I I I I I I I

    I I I I

    33

    3

    =−==−=

    =−=

    I#

    I%

    I&

    -I #%

    I#

    I%

    I&

    • n a ,-connected balanced 3-phase alternator* theline-currents are &.93 times the phase currents.

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    %alanced 3-"hase Loads

    a

    bc

    #

    %

    &

    #%

    %&

    N

    I#

    I%

    I&

    Ia

    IbIc

    • load is said to be balanced* i" all phase impedances

    are e%ual. Z

    A

    Z B

    Z C

    3-phase Y-connected%alanced Load. 8 #

    8 % 8 &

    a

    bc

    #

    %

    &

    #%

    %&

    N

    I#

    I%

    I&

    Ia

    IbIc

    Z C

    Z B

    Z A

    3-phase 7-connected

    balanced load. 8 # 8 % 8 &

    3-phaserecti9er

    3-phase inductionmotor

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    %alanced 3-"hase Loads

    a

    bc

    #

    %

    &

    23

    N

    I#

    I%

    I&

    Ia

    IbIc

    Z

    Z

    Z

    23 23

    3-phase#lternator

    %alance3-phaseload.8 : ; 0 L

    < =

    balance 3-phase load is connected to a 3-phase alternator withline-to-line voltage o" '3 volts. :ind7a) 8oad phase currentsb) 8oad line currentsc) ;hasor diagram o" phase and line currents.

    Illustrative "roblem '2

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    %alanced 3-"hase Loads

    a

    bc

    #

    %

    &

    23

    N

    I#

    I%

    I&

    Ia

    IbIc

    Z

    23 23

    3-phase#lternator

    %alance3-phaseload.8 : ; 0 L

    < =

    Z

    Z

    I#%

    I%&

    I

    8et74 / '3

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    %alanced 3-"hase Loads°−∠=−∠= 69.355.269.333055.2 AB I

    °−∠=−−∠= 69.12355.2)69.3390(55.2 BC I

    °∠=−∠= 116.3155.2)69.33150(55.2CA I

    33/,? o

    33/,? o

    3 3

    / , ?

    o

    I#%

    I%&

    I

    )( CA ABCA AB A I I I I I −+=−=

    )( AB BC AB BC B I I I I I −+=−=)( BC CA BC CAC I I I I I −+=−=

    I#

    I%

    I&

    33/,? o

    @,/3' o

    '

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    %alanced 3-"hase "ower

    a

    bc

    #

    %

    &

    #%

    %&

    N

    I#

    I%

    I&

    Ia

    IbIc

    Z C

    Z B

    Z A

    8 # 8 % 8 &

    B #%

    I#%

    I%&

    I#%

    '2 o

    '2 o '2 o

    %&

    3 o

    I#%

    I%&

    I

    B %&

    B

    CACAC

    BC BC B

    AB AB A

    I V S

    I V S

    I V S

    ===

    #pparent power perphase

    CACACAC

    BC BC BC B

    AB AB AB A

    I V Q

    I V Q

    I V Q

    φ

    φ

    φ

    sin

    sin

    sin

    =

    ==

    ;eactive power perphase

    CACACAC

    BC BC BC B

    AB AB AB A

    I V P

    I V P

    I V P

    φ

    φ

    φ

    cos

    cos

    cos

    =

    ==

    ;eal power perphase

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    %alanced 3-"hase "ower

    CACACAC

    BC BC BC B

    AB AB AB A

    I V Q

    I V Q I V Q

    φ

    φ φ

    sin

    sinsin

    ===

    ;eactive power perphase

    CACACAC

    BC BC BC B

    AB AB AB A

    I V P

    I V P I V P

    φ

    φ φ

    coscoscos

    =

    =

    =

    ;eal power perphase

    Cor balanced delta-connected load:

    P CA BC AB

    L P CA BC AB

    L P CA BC AB

    I I I I I

    V V V V V

    φ φ φ φ ===

    ====

    ====

    3

    CACAC

    BC BC B

    AB AB A

    I V S

    I V S I V S

    ===

    #pparent power perphase

    P P P P C B A

    P P P P C B A

    P P P C B A

    I V P P P P

    I V QQQQ

    I V S S S S

    φ

    φ

    cos

    sin

    ========

    ====;ASvalueonl notthephase

    alue onlnot thephase

    P L L P L

    L P P P T I V I

    V I V Q φ φ φ sin3sin3

    3sin3 =

    ==

    P L L P L

    L P P P T I V I

    V I V P φ φ φ cos3cos3

    3cos3 =

    ==

    L LT T T I V Q P S 322 =+=

    where:

    " phase volta!eL line volta!e

    I" phase currentIL line currentS " phase apparentpowerD " phase reactive

    power" " phase real

    Let:D total reactive power taEen b

    load" total real power taEen b loadS total apparent power taEen bload

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    %alanced 3-"hase "ower

    a

    bc

    #

    %

    &

    23

    N

    I#

    I%

    I&

    Ia

    IbIc

    Z

    Z

    Z

    23 23

    3-phase#lternator

    %alance3-phase

    load.8 : ; 0 L < =

    :ind the per phase apparent* reactive* and true power consumedby the load as shown by the fgure below.

    Illustrative "roblem '3

    A I I I I P CA BC AB 55.2====

    °= 69.33 P φ

    V AB V BC V CA V P '3 V

    VA I V S

    W I V P

    VAR I V Q

    P P P

    P P P P

    P P P P

    586.5)55.2)(230(

    0.48869.33cos)55.2)(230(cos

    33.32569.33sin)55.2)(230(sin

    ===

    =°==

    =°==

    φ

    φ

    KVAVA P QS

    W I V P

    VAR I V Q

    T T T

    P P P T

    P P P T

    76.15.759,1)24.845()49.563(

    99.146369.33cos)55.2)(230(3cos3

    99.97569.33sin)55.2)(230(3sin3

    2222 ==+=+=

    =°==

    =°==

    φ

    φ

    Solution7

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    %alanced 3-"hase "ower

    3-phase 9B.@ C5 delta-connected induction motor is suppliedby a 3-phase star-connected alternator generating & 4between phases. " the "ull load e ciency and the power "actoro" the induction motor are =' E and .F> respectively* calculateGa) !urrent in each motor phaseb) !urrent in each alternator phase

    Illustrative "roblem 'F

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    %alanced 3-"hase "ower

    3-phase* > AH* B&> 4 star-connected induction motor has anoutput o" > C5 with an e ciency o" = E and a power "actor o".F>. calculate the line current. " the motor windings are now

    connected in delta* what would be the correct voltage o" a 3-phase supply suitable "or the motor6

    SeatworE

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    %alanced 3-"hase "ower

    Illustrative "roblem'FTwo 3-phase balance loads a e connected in pa allel to a 400-! line. The "i stload is delta-connected with a phase i#pedance o" " # $0%&'0 and the second

    is a sta -connected p$ el% esisti&e load o" ( # 2) oh#s pe phase. 'inda) The phaso line c$ ents I A , I B , and I C .

    b) The appa ent, eacti&e, and eal powe cons$#ed b% the co#bined load.

    c) The ' o" the co#bined load.

    Z

    Z Z R

    R

    R

    A

    B

    C

    I A

    I B

    I C

    N

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    "hase Se uence

    N S

    "erspective view o+ armature

    N S

    Side view o+ armature

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    "hase Se uence

    N S

    "erspective view o+ armature

    N S

    Side view o+ armature (turned ? o )

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    "hase Se uence

    N S

    &' e

    deg

    N S

    # % &"erspective view o+ armature

    Side view o+ armature

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    "hase Se uence

    N S

    &' e

    deg

    N S

    # % &

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    "hase Se uence

    N S

    &' e

    deg

    N S

    # % &S$ S$D1$N&$ #%& % %

    V a

    V b

    V c

    ;hasor representation o"

    /! se%uence

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    "hase Se uence

    &' e

    deg

    N S

    # & %S$ S$D1$N&$ #&% &%# %#&

    IJ TKI# 5 1D 1LS #88M51D I#D 1T#I!A 1L#D

    V a

    V c

    V b

    ;hasor representation o"

    !/ se%uence

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    "hase Se uence

    &' e

    deg

    N S

    # & %

    phase se%uencedefnes which o" thethree phase voltages orline voltages comes inse%uence.

    There are only twopossible phasese%uence in three-phase

    system7 phase se%uence/! or phase se%uence!/.

    ;hase se%uence /! is

    called positive se%uence

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    "hase Se uence

    &' edeg

    N S

    # % &

    3-"G#S$ F-*I;$

    a

    bc

    #

    %

    &

    #%

    %&

    N

    N#N%N&N

    /

    !1

    3-phase F-wire alternatorwith output connected to

    lines #. %. &. H N

    3-phase F-wire lines

    1

    /

    !

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    "hase Se uence

    3-"G#S$ F-*I;$

    /

    !1

    ;hase se%uence /!7

    &' e

    deg

    N S

    # % &

    o P AN V V 0∠=

    o

    P BN V V 120−∠=o

    P CN V V 120∠=

    where V P is the line-to-neutral voltage

    or the phase voltage

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    &hecEpoint '

    /

    !1

    ;hase se%uence /!7

    &' e

    deg

    N S

    # % &

    o P AN V V 0∠=

    o

    P BN V V 120−∠=o

    P CN V V 120∠=

    where V P is the line-to-neutral voltage

    or the phase voltage

    Liven the phase se%uence o" phase voltages 4 1 * 4 /1 * and 4 !1 *

    below* what is the phase se%uence o" the line voltages* 4 / * 4 /! *4 ! 6

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    "hase Se uence

    3-"G#S$ F-*I;$

    /

    !1

    ;hase se%uence /!7

    &' e

    deg

    N S

    # % &

    o P AN V V 0∠=

    o

    P BN V V 120−∠=o

    P CN V V 120∠=

    o P AB V V 303 ∠=

    o

    P BC V V 903 −∠=o

    P CA V V 1503 ∠=

    where V P is the line-to-neutral voltage

    or the phase voltage

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    "hase Se uence

    3-"G#S$ F-*I;$

    /

    !1

    ;hase se%uence !/7

    o P AN V V 0∠=

    o

    P BN V V 120∠=o

    P CN V V 120−∠=

    o P AB V V 303 ∠=

    o

    P BC V V 1503 ∠=o

    P CA V V 903 −∠=

    where V P is the line-to-neutral voltage

    or the phase voltage

    &' e

    deg

    N S

    # & %

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    "hase Se uence

    3-"G#S$ 3-*I;$

    /

    !

    ;hase se%uence /!7

    &' e

    deg

    N S

    # % &

    o L AB V V 0∠=

    o

    L BC V V 120−∠=o

    LCA V V 120∠=

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    "hase Se uence

    3-"G#S$ 3-*I;$

    /

    !

    ;hase se%uence !/7

    o L AB V V 0∠=

    o

    L BC V V 120∠=o

    LCA V V 120−∠=

    &' e

    deg

    N S

    # & %

    where V L is the line-to-line voltage

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    Sin!le-"hase 3-*ire S stem

    n

    /N

    S

    N

    S

    n

    /&F e deg

    %n

    #n

    o P An V V 0∠= o P Bn V V 180∠=

    )sin(#a* t vv P An ω = )180sin(#a*o

    P Bn t vv += ω

    %n

    Bn An An An Bn AnnB An AB V V V V V V V V V 22 −==+=−=+=

    4 /

    F-pole alternatorwith 2 coils # H %

    &oils # H %. in series

    n

    4 n

    4 /n

    #n #%

    2

    2

    -

    -

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    :ind the currents and total power dissipation asshown in :ig. & and :ig. ' i" 4 n - 4 /n & 4.

    Illustrative "roblem

    ',

    Sin!le-"hase 3-*ire S stem

    n

    /

    n

    ? & 3 2 NB

    ? ' 3 2 NB

    /

    n

    n

    /

    n

    ? & 3 2NB

    ? ' 3 2 NB

    /

    n

    ? 3 3 2NB ? 3 3 2NB

    2

    2

    -

    -

    2

    2

    -

    -

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    :ind the currents and total power dissipation asshown in :ig. 3 4 n - 4 /n &> 4.

    Illustrative "roblem

    ',

    SeatworE

    n

    /

    n

    /

    n

    ?

    ? B 2 N>

    ?

    2

    2

    -

    -

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    $N OCS$SSION