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    CH APTE R 7 Proving Test of Duo bias Transformer

    Protection

    INTRODUCTION

    The use of unit systems of protection is now almost

    standard practice in all important electrical power sys-

    tems. M ost unit systems are of the balanced class and

    are based on the assumption that under through-fault

    conditions the currents entering and leaving the pro-

    tected zone are equal to one another, or bear some fixed

    relationship to one another. In applying unit protection

    to power-transformers two special problems arise, nam-

    ely, the unbalancing effect of tappings on the trans-

    former w indings w hich cause the relationship between

    the magnitudes of the input and output currents to vary,

    and the magnetizing inrush current which occurs when

    switching on a transformer with its output side open-

    circuited or very lightly loaded. The first problem is

    usually dealt with by employing bias or restraint on the

    relays so that the current required to operate the protec-

    tion increases roughly in proportion to the straight-

    through fault-current. The second problem presents

    much greater difficulty. It can be dealt with by introduc-

    ing time lags, as in conventional systems such as that

    using our type-TJG relay, or by methods which in some

    way or other differentiate between normal internal-fault

    currents and magnetizing inrush currents in such a way

    that the protection operates for the former but not for

    the latter. O ne difference between these two currents,

    which m ay be used for the purpose mentioned, lies in

    their wave-forms, fault-currents being nearly sinusoidal,

    whereas magnetizing currents contain appreciable sec-

    ond harmonic. The duo-bias system of transformer pro-

    tection derives its magnetizing stability b y taking this

    into account.

    GENERAL PRINCIPLES OF DUO-BIAS

    TRANSFORMER PROTECTION

    The principles of duo-bias protection are now fairly well

    known. It is a Merz-Price system with biasing to take

    care of tap-changing, and harmonic restraint to coun-

    teract the effect of magnetizing inrush currents. A

    schematic diagram for one phase of a three-phase trans-

    former is shown in fig. 1. It differs from most other

    differential systems of transformer protection in that the

    relay is fed from the secondary winding of a transductor,

    the primary winding of which is connected across the

    pilots in the usual way . Biasing is obtained by d.c. excita-

    tion of the transductor via a separate d.c. control-

    winding which is fed from an auxiliary transformer in

    series with the pilots. On internal faults the transductor

    acts more or less as a transformer but on external faults

    the saturation of the transductor core by the d.c.

    control-winding prevents the unbalance current present

    in the pilots from being transferred to the relay. W ith

    magnetizing inrush currents the harmonic-restraint cir-

    cuit has appreciable second-harmonic output. This is

    RELAY

    FIG. 1. DUO BIAS DIFFERENTIAL PROTECTION

    WITH TRANSDUCTOR RELAY

    rectified and fed into the d.c. control-winding on the

    transductor thus biasing the protection in the same way

    as does straight-through fault-current.

    Fig. 2 shows the interconnections between the relays

    in the protection of a three-phase transformer. It should

    be noted that the outputs of the three filter-units are

    paralleled and fed through the transductor bias-

    windings of all three phases connected in series, thus

    ensuring adequate restraint in all relays under condi-

    tions of magnetizing inrush.

    TESTS ON DUO-BIAS PROTECTION

    Research and exhaustive testing are continually finding

    new ways of improving the performance of protective

    systems generally. The Reyrolle Research and Certifica-

    tion Laboratories are very fully equipped for work of

    this kind and the majority of system conditions can

    readily be simulated. For transformer protection, how-

    ever, a fundamen tal difficulty exists in connection with

    the production of magnetizing inrush currents which

    represent service conditions sufficiently accurately. It is

    therefore desirable to supplement laboratory tests on

    transform er differential-pro tection with tests on site. It

    is not often that facilities for site tests are available but

    through the courtesy of the Central Electricity Author-

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    CVRRENT-TRANSFORrlERS

    ON PRIMARY

    POWER TRANSFORMER

    CRRENT.TRANSFORMERS

    ON SECONDARY

    TRANSDUCTORS

    SECOND HARMONIC

    FILTERS

    FIG. 2.

    PROTECTION 0~ A 3-~~4sE TRANSFORMER

    RELAY

    ity, Eastern Division, it was possible to test the duo-bias

    system thoroughly at their Rayleigh Transform ing Sta-

    tion recently and these tests, together with comprehen-

    sive laboratory tests, have fully proved the performance

    of the system. Before dealing with the site tests we give a

    brief outline of the laboratory tests.

    Secondary injection Tests

    A large num ber of tests were mad e using secondary-

    injection circuits, and these provided data on the trans-

    ductor and filter characteristics, and the ratings of com-

    ponents.

    A detailed investigation of the percentage-bias

    characteristic showed that the overall relay performance

    was almost unaffected by phase variations between the

    bias and the operating inputs to the transductor, and that

    the settings were similar irrespective of whether the

    inputs were switched or slowly increased. Further tests

    were made to determine the effects of harmonic content

    and frequency variations.

    The operating-time of the protection at three times

    the setting of the relays was shown to be approximately

    60ms. with no through-load current, and 85ms. with

    full-load current. Furthermore, it was proved that the

    asymmetry of the fault-current made little difference to

    the operating-time, the actual times varying by only 5ms.

    between fully symmetrical and fully asymm etrical condi-

    tions.

    The detailed data obtained by means of low-current

    testing techniques were confirmed by tests using primary

    injection as described below.

    Primary-injection

    Tests

    In order to simulate site conditions as closely as poss-

    ible, a number of laboratory tests were made using cir-

    cuits incorporating 500-kVA and 2500-kVA power-

    transformers.

    For the majority of the tests the transformer had a

    3-phase rating of 500-kV A, 660 /48 volts, with delta/star

    windings. On the H.V. (delta) side three 25/l current-

    transformers (i.e. 200/l using 8 primary turns) were

    connected in star, and on the L.V. (star) side three 600/l

    (i.e. 347 /0.58 ) current-transformers were connected in

    delta. With these ratios the steady-state unbalance cur-

    rent was negligible. To simulate power-transformer

    ratio-changes (due to tap-changing) of plus and minus

    12& , the number of primary turns used on the H.V.

    current-transformers was altered from 8 to 9 and 7

    respectively.

    Fig. 4 shows the magnetization curves of the current-

    transformers used in these tests, but other current-

    transformer designs have also been tested.

    Fault-settings without through-load were measured in

    terms of the H.V. current, and were less than 36 for all

    phase-to-phase and phase-to-earth faults, the variation

    in the settings obtained for the six fault-conditions being

    less than 5 . These figures applied for faults on both the

    H.V. side and on the L.V. side of the power-transformer.

    The effect on the fault-settings of 100 three-phase

    load (using the circuit shown in fig. 3) is shown in fig. 5,

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    FIG. 3. TEST-CIRCUIT LOAD

    AND

    FAULT

    CONDITIONS.

    from which it is apparent that the phase-angle between

    fault and load is unimportant in deciding the sensitivity.

    Tests also proved correct operation with high values of

    fault-current and current-transformer burden (such that

    the current-transformers saturated). The operating-time

    I

    I

    +_

    100

    CURRENT IA ,I I TIMES AVERAGE,

    FIG. 4.

    MAGNETIZATION

    CURVES

    OF

    THE

    CURRENT-

    TRANSFORMERS USED IN PRIMARY-INJECTION TESTS.

    of the protection is shown in fig. 6.

    The stability of the protection under through-fault

    conditions, the fault being applied on the secondary

    (L.V.) side after the transformer had been energized,

    was proved under normal and maximum tap-change

    conditions with H.V. current-transformer burdens of up

    to 8 ohms. Fig. 7 shows a typical record of the relay-

    operating current and L.V. primary current, the latter

    corresponding to approximately 15 times the current-

    transformer rated-current. The record shows the safety

    margin a t an extreme tap-change position, and illus-

    trates clearly that the relay output, resulting from the

    magnetizing current of the power-transformer prior to

    closure onto the fault on the L.V. side, is low relative to

    the relay operating-level. Tests were also made to

    demonstrate the stability when the H.V. side was ener-

    gized with an external fault already applied on the L.V.

    side, and to prove that repeated fault-current asymm etry

    did not prejudice the stability of the protection.

    Tests to prove the performance under conditions of

    magnetizing inrush current were made in the laboratory

    on the 500-kV A transformer and also on the 2,500-k VA

    6.6-kV 3-phase transformer. For the former, the ratio of

    the H.V. current-transformers was 200/l, and peak cur-

    rents of up to 6,l times the current-transformer rating

    were obtained, the time-constant of the magnetizing

    inrush current-decrement being 35m s (X/R = 11).

    These tests were made with repeated point-on-wave

    switching, and the protection remained stable through-

    out, oscillograph records showing that the value of the

    transient relay-operating current never exceeded half

    that required for operation. A further test was made

    using current-transformers of ratio 25/ 1, when the pro-

    tection remained stable with a peak magn etizing-current

    equivalent to approximately 30 times the current-

    transformer rating.

    Similar tests were made on the 2,500-k VA trans-

    former using 100 /l and 200 /l current-transformers of

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    27w

    FIG. 5. RED-PHASE-TO-EARTH FAULT-SE-ITING WITH 100

    PER CENT ~ PHASE

    LOAD.

    differing designs. Peak surges of up to 14 times the

    current-transformer rating and time-constants of

    105ms. were obtained on these tests.

    Site Tests

    The characteristics of duo-bias protection concerned

    with fault-settings and stability under through-fault con-

    ditions are independ ent of source-impeda nce and trans-

    former size. Stability under conditions of magnetizing

    inrush current is howev er depend ent upon both the

    magnitu de and the time-constant of the inrush current.

    The laboratory tests demonstrated the stability of the

    protection with heavy inrush currents but the time-

    constants of these inrush currents w ere much shorter

    OPERATING-CURRENT IN TERtlS OF tl LTlPLES OF FAULT-SETTING

    FIG. 6 OPERATING-TIME OF DUO-BIAS PROTECTION.

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    FIG. 7. RELAY-OPERATING CURRENT AND PRIMARY CURRENT UNDER THROUGH-FAULT CONDITIONS.

    than those usually associated with large power-

    transformers. The site tests at Rayleigh were made,

    therefore, to prove stability with an inrush cu rrent of

    long time-constant.

    The tests were made on 3O-MVA and 6Q-MVA

    132/2 2-kV transformers (see Table 1 opposite) using

    the current-transformers available on site. The

    magnetization-curves of these current-transformers are

    shown in fig. 9. It should be noted that these current-

    transformers have a much higher knee-point than those

    which would normally be supplied for duo-bias protec-

    tion. The use of these current-transformers does not,

    however, ease the test-condition, since here we are con-

    cerned with the output of a particular current-

    transformer (which will be higher the better the

    current-transformer) and not with the balancing of the

    outputs of current-transformers.

    Across the output of each power-transformer was

    permanently connected a 150-kV A aux iliary trans-

    former, the secondary winding of which was open-

    circuited. The magnetizing-current of this transformer

    would produce very little bias, and did not therefore

    affect the validity of the tests.

    Throug hout the tests Dud e11 oscillograph records

    were taken of the primary-current and relay-current in

    each phase, a nd the harmonic-bias current was recorded

    FIG. 8. CURRENTS DURING MAGNETIZING SURGE

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    Table l Data of Rayleigh Transformers

    Reference

    T3 T2B

    Rating

    I

    I

    1 30 MVA: 160 MVA:

    ON/OFB-cooled ON/OFB-cooled

    (15 MVA (30 MVA

    ON-rating)

    ON-rating)

    Connection

    Voltage

    Star-Delta

    132133 kV

    Star-Delta

    132133 kV

    1 Impedance

    1

    10.3

    1

    12.4

    Ratio of

    associated

    H.V. current-

    transformers

    15010.5

    25010.5

    on a moving-film cathode-ray oscillograph. Fig. 8 is a

    typical record and shows that the relay-current is well

    within the operating-level of the relay.

    Whereas the laboratory tests were made with control

    of asymmetry, thus permitting testing always under the

    most severe conditions of primary-currents, such control

    was not possible on site, and a large n umber of switching

    operations were necessary. A total of 69 switching oper-

    ations were made during these tests.

    In many tests the harmonic bias was deliberately

    reduced below its normal level by altering the primary

    turns on the harmonic-bias reactor, the bias produced

    being in direct ratio to the number of primary turns.

    Although the harmonic bias was reduced to 4 of its

    normal value protection still remained stable.

    Some of the more significant results are given overleaf

    in Tables 3 and 4.

    Examination of the results given above (and of the

    oscillograms taken) show that:

    (a) Th e greater the inrush current the greater the

    harmonic bias produced.

    (b) The greater the harmonic bias the less the relay

    current for corresponding inrush currents.

    (c) T he continuation of the asymm etrical wave due

    to the longer time-constant did not produce any

    adverse effect on the stability of the protection.

    CONCLUSION

    From the laboratory and site tests described it can be

    concluded that:

    1)

    2)

    Duo-bias protection is stable with through-fault

    currents of at least fifteen times the rated current

    of the current-transformers with magnetizing

    inrush surges having maximum peak values

    exceeding any likely to be found in practice, and

    also that it is stable with magnetizing surges hav-

    ing time-constants of at least 6 seconds.

    The fault-settings of the protection are less than

    40 per cent of the current-transformer rating with

    t

    FIG. 9. MAGNETIZATION CURVES OFTHE CURRENT

    TRANSFORMERSUSED IN SITE TESTS.

    no through-load, and less than 6 0 per cent of the

    current-transformer rating with 100 per cent

    three-phase through-load. The phase-angle bet-

    ween the load-currents and the fault-currents is

    unimportant.

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    Transformer No:-

    Steady-state Magnetization-current

    Time-constant

    Normal lead-burden

    Current-transformers-

    Ratio

    Secondary turns

    D.C. resistance

    Excitation curve

    Red and blue phases-l 1 A (approx.;

    Yellow phase 6 A (approx.,

    2 sets (approx.)

    4.6 ohms/phase

    3.4 A (approx.)

    6 sets (approx.)

    6 ohms/phase

    150/75/0*5 (used as 150/0.5)

    295 of 19 s.w.g.

    5 ohms

    Fig. 9

    Table &Results of Tests on Transformer T3

    Table 2-Site-testing Data

    T3 T2B

    25OlO.5

    495 of 19 s.w.g.

    3.5 ohms

    Fig. 8

    Nominal turns on

    harmonic-bias

    Table AResults of Tests on Transformer T2B

    Nominal turns on Lead-

    harmonic-bias burden

    reactor (per cent) (ohms/phase)

    Peak primary

    Relay-current Harmonic-

    current

    ( of operating-

    bias

    (A)

    current) current

    (m-Q

    Red

    Yellow Blue Red Yellow Blue

    I

    100

    I

    4.6

    1

    490 330

    1

    220

    1

    25

    1

    30

    1

    18

    1

    35

    1

    100

    4.6 230 320

    140

    21

    18 34 28

    57 4.6 570

    410 230 31 38 32 29

    57 6.6 340 180 160 30 25 28 9

    33 6.6 570 320 220 36 56 No record 8

    33

    6.6 110 120

    170 29 33

    27

    Very small

    (3) The operating-time of the protection is less than

    100 milliseconds at 3 times the setting under all

    conditions of load and fault-current asymmetry,

    and is less than 65 milliseconds at 3 times the

    setting for internal faults with no through-load.

    (4) The correct performance of the system is unaf-

    fected by the presence of harmonics higher than

    the second, and by departures from the nominal

    frequency greatly exceeding anything likely to

    occur in practice.

    These additional tests and appreciable operating

    experience with duo-bias protection have provided val-

    uable confirmation that this system of transformer pro-

    tection is basically sound in principle, and that it can be

    applied with confidence to the largest and most impor-

    tant transformers in service.

    127