Power Protecction course notes

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    Examples

    Problem 12.3

    The problem requires us to find the three

    currents Ia, Ib, and Ic, and also Vng.

    The network is symmetric. Therefore, the

    sequence circuits will be decoupled and we

    can analyze them one at a time.

    The zero sequence current must be zero

    since the source is ungrounded and thereforeIa+Ib+Ic=.

    !

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    "ut the gi#en #oltages are unbalanced. $o

    let%s hit them with an &'!to get the sequence

    #oltages as follows(

    =

    =

    +

    )*.

    ),!-.

    ,)))).

    !

    !

    !

    !

    !

    !!!

    )

    !

    *

    *

    jE

    E

    E

    ecall that for loads and transmission lines,

    /+=/'. $o we find the positi#e and negati#e

    sequence currents using the below circuits.

    0e obtain(=

    =

    + !*+11+.*

    ),!-.

    jI

    =

    = 2!**.

    *

    )*++.

    jI

    0e can then obtain the abc currents as

    =

    =

    ))).

    .!3,!-.

    .!31*-!.

    2!**.

    !*11.

    !

    !

    !!!

    *

    *

    c

    b

    a

    I

    I

    I

    4ow what about Vng5

    *

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    4otice from the positi#e and negati#e

    sequence circuits that =+ngV and =ngV .

    "ut consider ngV . The zero sequence circuit is

    6rom the zero'sequence circuit, a 7V8equation results in

    ==

    =+

    ,)))).,)))).

    ,)))).

    ng

    ng

    V

    V

    4ow we ha#e all of the symmetrical

    components of Vng, and we can therefore

    obtain Vngas their sum(=++=++=

    +,)))).,)))).

    ngngngng VVVV

    9larification( 0hen getting abc quantities

    from +' quantities, we hit the +' quantities

    with & :which contains terms in ; for the b'

    and c'phase quantities

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    quantities. &nd if we were to ha#e the c'

    phase +' quantities, then the c'phase

    quantity would ust be the sum of those c'phase +' quantities.

    roblem 12.17

    ecall that a 88> fault requires a parallel

    combination of all three sequence networks.$o we must find all ) sequence networks.

    ?seful comments about the below networks.

    0e get positi#e sequence phase shift of )@

    going from low to highA negati#e sequence

    of ')@ going from low to high.

    The problem requires pre'fault, phase a

    #oltage at the fault point be !.BC@.

    - The positi#e sequence network is the

    per'phase network for phase a. Therefore

    this !.BC@ lies in the positi#e sequence

    network.- Dre'fault implies no fault current, and

    since we are ignoring load currents, there

    is no current flow in the network.

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    - In the teEt, FE.!*.1, because the fault

    was on the line :in the middle of the

    diagram! and >*,

    the source #oltages had to be !BC')@.

    - Gere, because the fault is at the

    generator terminals, and therefore on the

    same side of the phase shift as >!, >!

    must be !BC@. "ecause there are equal andopposite phase shifts between the fault

    point and >*, >* must also be !BC@.

    The zero sequence network is

    - to ground at each gen since both gens are

    solidly grounded.

    - open between each gen and the network

    because of low side delta connection in the

    Efmrs.

    1

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    The fault point, at the terminals of >! :on

    the left

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    sequence, and it will be the pre'fault #oltage

    at the fault point, !BC@, for the positi#e

    sequence network.

    btaining the zero'sequence The#enin

    network is also easy because of the open

    circuit to the right of the fault pointA it is

    shown below.

    btaining positi#e, negati#e sequence The#.

    impedances requires analyzing networks

    with phase shifts. Gowe#er, because thephase shifts occur to #oltages and currents,

    The#enin impedances may be computed

    without consideration of phase shifts.

    This is true for what your teEt calls normal

    systems:see pp !1!'!1-

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    $o the positi#e and negati#e sequence

    networks to use in obtaining the The#enin

    impedances are below. 4ote that the positi#e

    sequence sources were idled.

    These are identical networks. Therefore the

    positi#e and negati#e sequence The#eninreatances are the same(

    !*,.

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    4ow we may draw the three The#enin

    equi#alent networks.

    &s mentioned at the beginning of thisproblem, a 88> fault requires a parallel

    combination of all three sequence networks.

    The connected circuits for analysis of a 88>

    at the >! terminals is shown below.

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    is easily done from the The#enin circuits

    and knowledge of the fault currents, as seen

    below.

    &s a check on this work, let%s take a look at

    the abc #oltages at the fault point.

    !!

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    =

    =

    =

    23+2.

    **3*.

    **3*.

    **3*.

    !

    !

    !!!

    *

    *

    c

    b

    a

    V

    V

    V

    Then we would use the sequence #oltages at

    the fault point, in each sequence network, tocompute the currents in the #arious

    elements. To do this, we would need to go

    back to circuits with the phase shifts :see

    page 2