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    PDC Measurements at Generator Bars

    C. Sumereder, M. Muhr, R. Woschitz

    Graz University of Technology

    Institute of High Voltage Engineering and System Management

    Inffeldgasse 18, 8010 Graz, Austria

    [email protected]

    Abstract: The dielectric response function of an

    electric insulation system can be determined by the

    measurement of the polarization and depolarization

    current (PDC). Beside partial discharge and dissipation

    factor measurements the time domain dielectric

    response function can be taken to gain information

    about the aging process and the condition of the

    insulation medium. The best results for the condition

    evaluation can be achieved at the frequency domain

    description in the shape of the complex capacitance and

    dissipation factor. For this reason the dielectric responsefunction has to be converted with the Discrete Fourier

    Transformation (DFT).

    Until now the PDC method was successfully applied to

    determine the water content of oil-paper systems in

    transformers. This paper should give a view to PDC

    measurements at insulation systems for rotating

    machines and the implication for the condition

    evaluation. First results of the diagnosis with the PDC

    method are discussed and a comparison to classical

    dielectric measurements is given.

    Dielectric Measurements at Generator Bars

    Dielectric measurements are a very important tool to

    evaluate the condition of electric insulation systems,

    different standards were state of the art, e.g. the testing

    of the insulation resistance [1] or the dissipation factor.

    The test methods can be divided in AC tests with (0.1)

    50/60 Hz or higher and DC methods.

    Figure 1: Equivalent circuit and DC currents for

    insulation systems [1]

    The most popular dielectric measurements were

    dissipation factor, insulation resistance (polarization

    index) and partial discharge test. Beside these there

    were also the absorption (polarization) current,

    conduction current, geometric capacitance current andsurface leakage current. Figure 1 shows the equivalent

    circuit of an insulation system and the measured

    currents during insulation resistance test according to

    [1].

    The total current of insulation resistance measurements

    is the sum of leakage, conductance, capacitance and

    absorption current, according to equation {1}. The

    quantitative characteristic of each is illustrated in

    figure 2.

    IT = IC + IG + IL + IA {1}

    Figure 2: Types of currents at DC resistance

    measurement of insulation systems [1]

    The absorption current decays at a decreasing rate. The

    current vs. time relationship is a function according to

    equation {2}; it may be plotted as a straight line on a

    double logarithmic scale graph.

    IA = K. t n {2}

    IA absorption Current

    K function (insulation system, test voltage)

    t time of applied direct voltage

    n characteristic function of insulation system

    The absorption current consists of two components,

    which are due to the polarization of the impregnating

    materials and the gradual drift of electrons and ions

    through most organic materials. Organic molecules,

    such as epoxy, polyester, and asphalt, tend to change

    orientation in the presence of a direct electric field. It

    usually takes several minutes after application of the

    electric field for the molecules to become reoriented.

    Proceedings of the XIVth International Symposium on High Voltage Engineering,

    Tsinghua University, Beijing, China, August 25-29, 2005

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    The conduction current in well-bonded polyester and

    epoxy-mica insulation systems normally is zero unless

    the insulation has become saturated with moisture.

    The surface leakage current is constant over time, where

    a high level can be caused by moisture or some othertype of partly conductive contamination present in the

    machine.

    The quantity of each current is dependant of the used

    insulation materials and factors as geometrical

    arrangement. The characteristic of the total current

    admits statements about the condition of the insulation

    system. E.g. a low percentage of the leakage and/or

    conduction current can be interpreted as cleanliness and

    dryness, if the windings were wet or contaminated the

    absorption current is relatively smaller. For clean and

    dry rotating machine insulation, the insulation

    resistance is between about 30 s and a few minutesprimarily determined by the absorption current.

    Dielectric Response Function

    The measurement of dielectric response function and its

    interpretation for the condition evaluation is a very old

    method. Beginning in the year 1889 [2] physicist started

    to investigate the polarisation and depolarisation

    behaviour of insulants. In 1927 a contribution about the

    anomaly of dielectrics was mathematical described. The

    so called Curie - von Schweidler Law [3] describes the

    dependence of currents during polarization and

    depolarization as linear function in double logarithmic

    scale. The theory and results from measurements are

    shown in figure 3.

    Figure 3: dielectric response function in theory and real

    The dielectric response of an electrical insulation

    system at the PDC method is measured in time domain.

    The polarization and depolarization current in

    dependence of time is recorded, transformed and

    evaluated. Several measurements have shown that the

    so called Curie - von Schweidler law does not meet thisbehavior in real, because dielectrics were heterogeneous

    systems. The characteristic of the polarization

    behaviour depends on the geometry and insulation

    conditions.

    The time domain response function is converted to the

    frequency domain description, the Discrete Fourier

    Transformation (DFT) is applied [4]:

    00

    )()(

    UC

    titf d

    =

    = dtetff tj )()(

    The advantage of this mathematical procedure is that

    the frequency domain is a complex description of the

    response function where the parameters conductivity,

    permittivity and polarization can be described according

    to the formula:

    =

    +

    =+=

    rrr

    r

    rPOLL

    j

    *

    0

    0tantantan

    {3}

    with: conductivity, tan dissipation factor, r* complex permittivity

    The dissipation factor can be expressed according to

    {3} where the conductivity and the real part of the

    complex permittivity show a very low dependence to

    frequency. The imaginary part has a strong dependence

    to frequency caused of different polarization mechanism

    in the insulating medium. The results of a simulation for

    the variation of the parameters , c and c areillustrated in figure 4 and 5. The rise of the conductivitycauses a change in the shape of the tan function in thelower frequency area. The process of a rising

    conductivity should be characteristic for degradation of

    the insulating medium. The rise of c and c proceeds

    in the opposite way. A rising of c, which can be

    interpreted as a rise of the relative permittivity, causes a

    parallel decrease of tan and vice versa for c.

    Figure 4: Variation of dissipation factor in dependence

    of conductance

    Up to now there were many considerations done about

    possible connection between the dielectric relaxation

    Proceedings of the XIVth International Symposium on High Voltage Engineering,

    Tsinghua University, Beijing, China, August 25-29, 2005

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    and condition or residual disruptive strength of the

    insulation medium, but all this expectations could not

    be fulfilled, no physical parameter is known which can

    represents an absolute parameter. For this reason the

    dielectric parameter and r were taken into accountfor the evaluation of the measurements.

    Figure 5: Variation of dissipation factor in dependence

    of parameters c and c

    Taking a look to the equivalent circuit of the generator

    bar insulation several serial and parallel resistances and

    capacitances can be observed (pancake model). This

    insulation system is built of two components: mica tape

    and resin. The R0 represents the geometric resistance,

    C0 the vacuum capacitance and Ri, Ci the polarization

    mechanism. The size of these parameters is determined

    by the proportion of the used components. The per cent

    by volume of mica at resin rich bars is about 70% and at

    VPI bars 85-95%. The dielectric strength is mainlydestined by the electric field strength and the resulting

    voltage distribution. Figure 6 illustrates the electric field

    strength in the material components resin and mica tape

    (left) and the equivalent circuit with the parallel linked

    geometric resistances and vacuum capacitances (right).

    Figure 6: Dielectric model of a generator bar and

    equivalent circuit of heterogeneous dielectrics

    This equivalent circuit meets the theory of the Maxwell

    two-layer model: The dissipation factor is dependant on

    the temperature and the power frequency for a dielectric

    with orientation polarization; a temperature rise isequivalent to a decrease of the power frequency. A

    higher temperature disturbs the orientation process as

    well as the dipoles can not follow the field at high

    frequencies [5]. The parallel linked Ri and Ci describe

    further polarization effects, Ri delays the polarisation

    and depolarisation processes of the serial linked Ci.

    Test Objects and Measurements

    The test objects are generator bars of resin rich

    technology. The generator bars were in operation in

    different periods of time. The preparation of the test

    objects and arrangement of the measuring equipment

    can be seen in figure 7. The PDC measurements were

    done periodically approximately all 100 h.

    CXTest Voltage

    Grounded Electrodes

    Measuring Air Gap

    Electrode

    Figure 7: Preparation of generator bars and connection

    of power supply test lead for dielectric measurements

    The air gap was necessary to separate the geometric

    resistance and vacuum capacitance of the total

    resistance and capacitance values (with generator bar

    ends) on the one hand and on the other to prevent

    leakage currents.

    Results

    For the evaluation of the test results the polarization and

    depolarization currents, the complex capacitance,

    insulation resistance, dissipation factors were

    investigated in detail. In diagram 1 the depolarization

    currents of one generator bar in dependence of load

    time was observed. The current shows an almost linear

    decreasing characteristic. In dependence of load time

    the Depolarization current were rising.

    Diagram 1: Depolarization Currents

    In diagram 2 the insulation resistances of the same

    generator bar were shown in dependence of load andmeasuring time. The Resistances were calculated:

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    Tsinghua University, Beijing, China, August 25-29, 2005

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    IR = Uc/IPOL, IR = Uc/(IPOL-IDEPOL), in the diagram the

    R values are illustrated because of the very small

    differences between R and R. From this diagram the

    Polarization Index (PI) could be calculated. For all

    curves the PI was within the demanded values

    according to the standard [1]. According to the Current

    measurements the insulation resistances had the similar behaviour. In dependence of load time the resistances

    get smaller and smaller.

    Diagram 2: Insulation Resistances

    In diagram 3 the real part of the complex capacitance is

    shown. The c rises with load time in the lower

    frequency areas. At higher frequency there was almost

    no change in quantity.

    Diagram 3: Complex Capacitances, Real Part

    The processes of aging concerning the imaginary part of

    the complex capacitance is shown in diagram 4. The

    curves rise with load time over the whole frequency

    area. The dissipation factor in dependence of load time

    is illustrated in the diagram 5. The curves show a risingbehaviour with load time over the total frequency area.

    Diagram 4: Complex Capacitances, Imaginary Part

    Diagram 5: Dissipation Factors

    Conclusions

    The results of the PDC measurements and the

    calculation of dielectric parameters can be summarized

    as follows:

    The theoretical considerations about the behaviour of

    dissipation factor in dependence of resistivity and

    complex capacitance were met very well. The resistance

    of the generator bars falls, the complex capacitance

    raised with load time. The mathematical formulation of

    dissipation factor according to equation 3 is confirmed.

    It was observed that the generator bars fail out without

    sudden. This behaviour can be interpreted that the

    mechanism which causes the damage and finally the fall

    out happens very fast.

    With the PDC method the aging behaviour of anelectrical insulation system can be observed. It is an

    integrative method, for this reason no absolute

    statements (as a withstand voltage test or PD

    measurement enables) about the condition of the

    observed system can be done. It is important to do

    periodical measurements.

    The PDC method can be applied at generator bars in

    general. The application to measure a whole winding

    respectively a whole generator has to be verified. Future

    measurement should show

    References[1] IEEE Std 43-2000, Recommended Practice for

    Testing Insulation Resistance of Rotating Machinery

    [2] J. Curie, Recherches sur la Conductibilite des Corps

    Cristallises, Annales de Chimie et de Physique, 1889

    [3] E. von Schweidler, Studien ber die Anomalien im

    Verhalten der Dielektrika, Annalen der Physik 1907,

    24, 711-770

    [4] A. Helgeson, Analysis of Dielectric Response

    Measurement Methods and Dielectric Properties of

    Resin-Rich Insulation During Processing, Doctor

    Thesis, Kungl Tekniska Hgskolan Stockholm Sweden,

    2000, ISSN 1100-1593

    [5] A. Kchler, Hochspannungstechnik, VDI Verlag1996, ISBN 3-18-401530-0

    Proceedings of the XIVth International Symposium on High Voltage Engineering,

    Tsinghua University, Beijing, China, August 25-29, 2005

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