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    A New Selective Transient Protection for the Ground

    Fault of Large Unit-connected Generators

    Bi D a q ia ng , W a ng We i j i a n , Gui Lin a nd Wang

    Xiangheng

    Abstract-Based on the mu lti-loop circuit method of A C

    machine a mathematic model is established for the large

    unit-connected generators, namely the outlet terminal o f

    generators connected to a common busbar, and the transient

    zero-sequence current and voltage of these generators are

    simulated and analyzed at different grounding location. Further,

    making use of the wavelet transform sensitively detecting the

    singularity o f signal, the properties o f their value of wavelet

    transform are analyzed, and a selective transient protection is

    proposed according to the sign and value of the modu lus maxima

    o f wavelet transform. The results o f simulation and experiment

    verify the new p rotection can correctly detect the gene rator with

    ground fault, and discriminate between the internal and external

    Faults.

    Index Terms--generator, 'ground fault, zero-sequence

    componen t, transient protection, wavelet transform

    1. INTRODUCTION

    enerator stator is most frequently subject to the damage

    G aused by the ground faults, and they often precede other

    worse winding faults such as turn-to-turn and phase-to-phase

    faults, therefore ground-fault protection is the key element of

    the protection system for generators [4]. At present, the

    protection sch emes against the ground fault mainly include the

    zero-sequence fundamental voltage scheme, the third

    harmonic voltage schem e and subharm onic voltage injection

    scheme, their combination

    can

    provide 100 coverage of

    stator windings.

    But these schem es aren't able to discriminate which

    generator suffers the ground fault if several medium or

    small-sized generators are connected to the common busbar.,

    And they also can't distinguish between an internal and

    external .ground fault for

    a

    unit-connected generator. To avoid

    the unnecessary stopping of no-fault generator in the large

    unit-connected generators, it is desired for the protection

    scheme w ith selectivity.

    In fact, when a fault occurs, some relevant signals appear

    singular. These transient signals contain extensive fault

    information such as type, direction, location and sustained

    time. The information covers the entire frequency domain

    including DC, power frequency and high frequency [l].

    Extracting and utilizing these transient information can

    provide a new way to resolve the problem about the selectivity

    of protection scheme.

    This paper establishes a mathematic model for several

    circuit method of AC machine, transient zero-sequence current

    and voltage of these generator are simulated and analyzed

    under this model o f connect at different grounding location, a

    selective protection

    is

    proposed by using the wavelet

    transform to extract these transient information.

    11. ESTABLISHINGHE S l M UL Al l ON MODEL

    A. Assuming

    Condi t ions

    The diagram of large unit-connected system

    is

    showed in

    Fig. 1. In the procession of establishing the simulation model

    of whole system, self-conduction and mutual-conduction of

    generator windings are calculated by using the multi-loop

    circuit method of AC m achine [5]. Th e distributed capacitance

    of stator winding to ground is substituted by several lumped

    capacitances with uniform distribution along the stator

    windings, and the additional capacitance

    at

    terminal, low side

    winding capacitance of step-up transformer to ground and the

    grounding impedance on neutral are considered. The step-up

    transformer is represented by its equivalent circuit.

    At present the neutral of generator mainly grounded

    through Petersen coil or resistor, the variation o f stator current

    caused by ground fault is so small that the damping winding

    can be ignored during simulation, which means a generator

    with damping windings can be regarded as a non-damping

    windings generator during the ground fault.

    L

    L

    Fig. I. he diagram oflarge unitsannected

    system

    B.

    Establishing

    the

    state

    equations

    Choosing the current of inductance and the voltage of

    capacitance as the state variables, the last form of state

    eouations

    is

    derived in

    n

    trix

    as

    follows.

    l ~ ~ ~ ~ ~ ~

    generators connected to a comm on busbar using the multi-loop

    The

    authors are with the department of Electrical E ngineering and Applied

    Electronic Technology, Tsinghua University, Beijmg 100084 China (e-mail:

    bidaqiang990mails.tsinghuaeducn .

    where,

    p M + r

    A

    I

    =[-

    B

    F][U]+[ ]

    0-7803-7459~2/0~ 17.002002

    EEE

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    p

    is the differential operator;

    M C and r is the inductance, capacitance and resistance

    matrix of .generator winding s, terminal and neutral

    respectively;

    A

    and B are the associated matrix between node and

    branch;

    U s the vector of voltage source;

    and

    U

    re the vector of state variables;

    F is the associated matrix of between the fault node and

    branch, under normal condition

    F

    =

    O]

    when ground fault

    occurring, a zero element on the leading diagonal ought

    to

    be

    substituted by

    - l / R g

    according to the fault location, here

    Rg

    is the transient resistance.

    111. SIMULATION

    ND

    ANALYSIS

    Using the above mathematic model, this part simulates a

    system, which includes two same generators (No.1 and No.2)

    connected to the common busbar. Their main data are as

    follows.

    Rated power lZkW, rated voltage

    400V,

    pole pair number 2,

    parallel branches per phase 2, coil number per branch 7,

    excitation current under no-load and rated voltage 8.24 A, rated

    excitation current 22.6A. For genera tor 1 and generator 2, The

    capacitance of stator windings to ground is 0.12 P F and

    0.08

    P F and the additional capacitance at terminal is 0.03 P F and

    0.02

    P

    F respectively. The neutral is grounded through the

    Petersen coil and resistor with small value in series. The

    sampling frequ ency is

    IO .

    Two typical faults, occurring inside and outside generator,

    are simulated and analyzed. Defining

    io

    and io2 is the

    zero-sequence current of generator

    1

    and ,2, and uo is the

    zero-sequence voltage of the busbar.

    Fig. 2(a) gives the simu lation results of

    io o

    and

    u

    when

    a ground fault takes place at 42.9 of the first branch of A

    phase of generator 2 close

    to

    the neutral via

    5000

    transient

    resistance. It is showed the tran sient zero-sequence current and

    voltage is discontinuous, and the direction of change between

    h a n d

    io2

    is contrary after the ground fault occurring. Because

    the zero-sequence current through the outlet terminal of the

    fault generator is equ al to the all grou nd capacitance current of

    external voltage network expect that of itself, the transient

    zero-sequence current of the fault generator is greater than that

    of the normal generators, which can be seen from Fig. 2(a).

    Fig. 3(a) shows the s imulation results of an external ground

    fault at

    K,

    n Fig.

    1

    through

    500 R

    transient resistance.

    io

    and

    io change in the same direction, and uo produces a sharp

    change during the transient. Because the ground fault

    is

    outside generators,

    u

    has a larger variation than normal

    condition.

    In

    this case, the zero-sequence currents through the

    outlet terminal of generators are the ground capacitance

    current

    of

    themselves individually.

    IV.

    SELECTIVE ROTFCTIONSCHEME For GROUNDAULT

    A . Analysis of the wavelet transform

    Conventional Fourier transform can only give the

    information in frequency domain and has no ability of time

    resolution so that it is not fit to analyze the transient signal,

    and cant detect the singularity of signal in time field. Rather

    than as a developing time-frequency method, the wave

    transform is a powerful

    tool

    in proces sing the transient signal

    because of its ability to extract information from transient

    signal simultaneou sly in both time and frequency domain.

    According to the s ingularity detection theory of the wavelet

    transform [2] and [6], if a sudden change or discontinuation of

    signal appears, its wavelet transform values have the local

    modulus maxima, which

    carry

    some important information.

    The fault type and location can be discriminated by

    comprehensively using the sign and value of these local

    modulus maxima. This paper chooses Daubechies 5

    orthogonal wavelet as the mother wavelet and adopts the.

    atrous algorithm [3] to analyze the zero-sequence components

    by the detection of singularity with m ultiscale transforms, and

    the values of wavelet transform at scale 2 are used in the

    protection scheme at the sampling frequency IOkHz. Here

    WTI, and WTUo are defined

    as

    the values of wavelet

    transform of zero-sequence current of generator

    i

    and

    zero-sequence voltage of busbar respectively.

    During the normal condition, the variation of WTI WTI

    and W Uo is very flat in Fig. 2(b). But when the ground

    occurring inside generator 2, their values sharply change and

    there are the modulus maxima. Compared with the results of

    transform, the modulus maxima of WTI a n d . WT12 occur

    simultaneously and have the same sign. The value of the

    modulus maxima of

    WTI

    is more than that of W I Z .

    When the ground fault happening outside generators, there

    appear the modulus maxima of the zero-seq uence components.

    Comparing the results of transform, the modulus maxima

    occur simu ltaneously but their signs are contrary in Fig. 3(b).

    B.

    Elective p rotection scheme

    Through the above analysis, the elective protective scheme

    is advancedas follows,

    1) Choose the values of the wavelet transform of the

    zero-sequence current and voltage of generators at scale 2 as

    the characteristics of ground fault at the lokHz sampling

    frequency;

    2 ) Calculate the modulus maxima WTI,,k of zero-sequence

    currents (including the positive and negative,

    i = l - n

    is the

    number of generator, k

    is the

    position of maximum . If the sign

    of mI h of generator i is contrary to that of all other

    generators, then the ground fault occurs inside a generator;

    (3)

    Under the condition 2, if the number of generators

    connected together is more than 2, then generator

    i

    is the fault

    generator. When there are only

    two

    generators, if

    IWTI I

    is

    greater than that of the other generator additionally, then the

    generator i is the fault generator;

    (4) If all of sign

    is

    identical amon g WTIj,i

    i= l -n ) ,

    then the

    ground fault is external;

    5 ) To improve the reliability of detecting external faults,

    supplement

    I W T I I , k I > W T I , , .

    For the external ground fault,

    the range of the zero-sequence voltage variation

    is

    very large,

    so that the value of W U,*,is easily

    set;

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    'I

    021

    (a) Transient zero-sequence comp onents

    4

    os

    I

    019

    0 2

    021 022 on ou

    2s

    t ( 3 )

    (b) The results of wavelet transform

    at

    scale

    2

    Fig.

    2 The simulationresultsof

    an

    internal pound fault

    (6) To enhance the reliability of whole protection scheme,

    only after more than three points of the modulus maxima

    continuously meet the conditions, the protection scheme

    decides whether and where the ground fault happens.

    V. RESULTS O F WERIMENT

    To verify the above elective protection scheme, some

    experiments were carried on a large unit-connected system

    with

    two

    generators, an d its diagram likes Fig.

    1.

    The main

    data of

    two

    generators are

    as

    follows.

    Generator]: rated capacity

    5.0kW,

    rated voltage 400V. pole

    pair number 2, parallel branches per phase 1, excitation

    current under no-load 0.162A, the capacitance of stator

    windings to ground 0.048 E Ge nera tor2 rated capacity

    3.75kW, rated voltage 400V. pole pair number 2, parallel

    branches per phas e 1, excitation current under no-load 0.357A,

    the capacitance of stator windings to ground 0.036 E

    (a) Transient zero-sequence com ponents

    -319

    62 O i l

    oi2

    o

    ob

    ais

    C 4

    (b)

    The results of wa ve la transform at sede 2

    Fig 3

    The imulstlon

    resulls o fan external

    p o u n d

    fault

    There are 6 taps (25 . 33.3 , 41.7 , 45.5 , 47.7 and

    49.2 close to the neutral) on the windings of phase A . The

    neutrals of two generators are grounded through the potential

    transformer, and their outlet terminals are connected to 800V

    high voltage system via a step-u p transformer. The record data

    is via two level current and voltage transformer at lo&

    sampling frequency.

    The zero-sequence current of two generators and

    zero-sequen ce voltage of busbar are given in Fig. 4(a) when a

    solid ground fault

    occurs

    at terminal of generator

    2

    K2

    n Fig.

    1). Fig. 4(b) shows the results of the wavelet transform, their

    properties are consistent with th e analysis of simulation results

    in part IV. The values of wavelet transform at the time of

    ground fau lt are distinctly higher those at normal time or the

    zero-sequence components. The sign of the

    modulus

    maxima

    between io] and io2is contrary, and the am plitude of the latter

    is higher than that of the former at scale 2.

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    (a) Transient zero-sequence components 8) Transient zero-sequence omponents

    2-

    In Fig. 5(a) the location of ground fault (K, in Fig. 1)

    is

    external, correspondingly

    it

    can be seen that at the scale 2 the

    sign and position

    of

    the modulus maxima of iol accords with

    that of iO2from ig. 5(b), and

    u0

    has modulus maxima too.

    lfthe fault location

    is

    close to the neutral

    K ,

    n Fig.

    I ,

    the

    scheme still can work, because the deviation voltage exists on

    the neutral, and the zero-sequence current and voltage still

    produce the transient w hen a ground fault occurring.

    VI. CONCLUSIONS

    Usual protection schemes against the ground fault cant

    realize the selectivity protection for the large unit-connected

    generators. Based on the simulation and analysis of this

    connect model established by the multi-loop circuit method, a

    new and selective protection scheme

    is

    presented. It uses

    Daubechies

    5

    orthogonal wavelet

    to

    detect the singularities

    of

    zero-sequence current and voltage, further utilizes the sign and

    amplitude

    of

    the modulus maxima

    to

    realize the selective

    protection. The experimental results verified the s electivity

    VII.

    RFERENCES

    Periodicals:

    [ ]

    Bo Zhiqian, Transient based protectio- new generation

    of

    power

    system protection, Power Syilem

    Technology

    ~01.20, a.3, pp. 34-36,

    1996.

    Stephane

    Mallet

    and WenLiang

    Hwang, Singularity

    detection and

    Processing with uwelets,

    IEEE T r am ln orormorion 7heory. Vo1.38,

    Na.2,pp. 617-643,Mar1992.

    Mark

    J.

    Shenra, Wedding the ~ U O Y S nd the Mallet algorithm, IEEE

    Trow.

    SignalProcessing, Va1.40,No.10, pp. 24642482,,Oet.1992.

    121

    [3]

    Books:

    [4]

    [SI

    Wang Wcijan, Principle

    and

    mpplication

    o

    electne power

    equipmenr

    proleclion

    Beijing: China Electric

    Power

    Press,

    1998,

    pp. 200-203.

    Gao Jingde, Wang Xiangheng,

    Li

    Fahai,

    Anolpir of

    altemrive cumm

    machine

    and

    { s

    system Beijing: Tsinghua University

    Press, 1994,

    Yang

    Fusheng,

    7he

    engineering

    mly>is

    and application

    o

    wovelet

    lronsform,Beijing: Science

    Press,

    2000, pp.

    145.157,

    pp.l-43.

    161

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    VIII. BICGRAPHIES

    Bi Daqiang was born

    in

    Jilin Province, China,

    on December

    20,

    1973. He received his M.S.

    degree in Electrical Engineering from Shenyang

    University of Technology

    in

    1996 Now he is

    pursuing his Ph.D. at Tsinghua University His

    field of interest mainly is the relay protection of

    main equipment in

    power

    system.

    Wm g Weijim was barn in Jiangru Province

    of

    China in 1930. He graduated

    from

    Electric

    Engineering DeparUnent of Tsinghua University

    in

    1955. Now he is a professor in the Department

    of Electrical Engineering, Tsinghua University

    He has

    been

    researching and teaching on

    the

    r e l w protection for large electric machine

    Cui Lin was

    barn in

    Anhui Province, China, on

    July 16, 1974. He received his

    B.S.

    and M.S.

    degree in Electrical Engineering from Hefei

    University of Technology in 19 and 1999.

    Now he

    is

    pursuing his Ph.D. at Tsinghua

    C ~ ~ $ s v -

    University His research interests are the analysis

    I?

    . . and relay protection of internal fault of

    -.

    t large-sized generators

    W m g Xiangheng

    WBS

    born in Anhui province of

    china, an October 19, ,1940. He gradua ted from

    Electrical

    Engineenng Depanment of Tsinghua

    University in 1964. He worked

    at

    Dongfang

    Electric Machine Works

    in

    Sishuan Province

    from 196 8 to 197 8 and obtained his P.h D

    diploma from Tsinghua University in 1986. He s

    currently

    a

    professor at Tsinghua University His

    presently conducts research

    on

    the analysis and

    wnbd

    for electric machine and its system, fault

    analysis and i ts protection for electric machine.

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