Fault Analysis in Four-wire Distributed Networks

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    BY:

    MD ABDUL RAHEMAN

    UNDER THE GUIDENCE OF:

    M N SUNEETHA

    R.M. Ciric, L.F. Ochoa, A. Padilla-Feltrin and H. Nouri, Members, IEEE

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    Fig. 1. Three-phase four-wire line section, considering ground.

    where

    a, b, c phase lines;

    n neutral wire;g ground.

    5x5 impedence matrix

    POWER FLOW ALGORITHM

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    A. Model

    Fig. 2. Model of the three-phase four-wire multi-grounded distribution line.

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    B. Power Flow Algorithm

    At iteration k:

    1. Nodal current calculation

    WhereIia, Iib , Iic,Iin , Iig are the current injections at node i;

    Sia, Sib, Sic, are scheduled (known) power injections at node i;

    Via, Vib , Vic , VinVig are voltages at node i;

    Yia Yib, YicYin, Yig admittances of all shunt elements at node i;

    Zgri grounding impedance at node i ( Zgi = Zgri+ Zggi )

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    2) Backward sweepsection current calculation

    Where

    current flows on line section ;

    M set of line sections connected downstream to node j .

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    3) Forward sweepnodal voltage calculation

    . Voltage Correction:

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    Convergence Criterion:

    the power mismatches at each node for all phases, neutral wire, and ground arecalculated as

    Flat Start:

    The initial voltage for all nodes should be equal to theroot node voltage

    If the real or imaginary part of any of the power mismatches is greater than a

    convergence criterion, steps 1, 2, and 3 are repeated until convergence is achieved.

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    SHORT-CIRCUIT ANALYSIS

    The hybrid Thevenin equivalent is calculated from:

    General fault boundary conditions in a 5x5 network representation for calculatingdifferent types of fault are given as:

    Where

    Vt is the voltage mismatch vector from (7)Vf

    (s) is the scheduled voltage (fault boundary condition)

    Vf(0) is the pre-fault voltage at the faulted node

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    Thevenin compensation impedance matrix Zt is determined in the form of a3x3-network representation.

    Hence, boundary fault conditions for Vf(s) are kept in 3x3 notation.

    solving fault currents It by (7),

    Node current injections of phases a, b and c = post-fault current injections + pre-faultnode current injections.

    The pre-fault node current injections of phases a, b and c are determined frompower flow solution.

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    For three-line-to-ground faults, at a three-phase line section, post-fault currentinjections are given by:

    whereIfa

    (p) , Ifb(p), Ifc

    (p) are post-fault phase current injections

    Ita, Itb, Itc are fault currents obtained by solving (7).

    For double-line-to-ground faults or line-to-line faults, on phases b and c, post-

    fault current injections can be If(p)

    formed by

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    For single-line-to-ground fault on phase a, post-fault current injection If(p) is

    determined from

    Post-fault node current injections of the neutral wire and ground are thencalculated using

    where

    Ifn(p)

    , Ifg(p)

    are post-fault neutral wire and ground current injectionsZgrfis the grounding impedance at the faulted node

    Znnf, Zggfare neutral wire and fictitious ground conductor impedances in thefaulted section (Zgf=Zgrf+Zggf).

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    CONCLUSION

    In this paper a method for fault analysis in four-wire DNs is discussed.

    In this paper, a power flow algorithm for three-phase four-wire radial DNs,considering neutral wire and multigrounding, is proposed.

    High-order line models (4x4, 5x5 and higher) may easily be added to acommon solution method for three-phase power flow.