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8/3/2019 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.