Tutorial discussion on Transient assessment

Transients are divided into two categories which are easy to identify: impulsive and oscillatory. If the mains signal is removed, the remaining waveform is the pure component of the transient. The transient is classified in the impulsive category when 77% of the peak-to-peak voltage of the pure component is of one polarity. Each category of transient is subdivided into three types related to the frequencies contained. Each type of transient can be associated with a group of phenomena occurring on the power system.

The impulsive low-frequency transient rises in 0.1 ms and lasts more than 1 ms.. Its companion, the oscillatory low-frequency transient, contains frequency components up to 5 kHz. These types are the most common transients recorded on a power system. They are not only easily propagated but they can also be amplified by a power-system resonance phenomenon. Measurement of these types of transients should be useful for all classes of application (benchmarking, legal, trouble shooting and laboratory)

The medium-frequency impulsive transient lasting between 50 ns to 1 ms and oscillatory transients between 5 and 500 kHz are less frequent than the low-frequency types but have much higher amplitude. These transients may not propagate as easily as the low-frequency types but may cause arcing faults on the power distribution system which result in voltage sag on many user power systems. It is most appropriate to measure these types of transients for trouble shooting and laboratory classes.

High-frequency types with high amplitude can be observed only near where the phenomenon occurs. The high-frequency impulsive transient has duration below 50 ns and the frequency of the high frequency oscillatory type ranges between 0.5 and 5 MHz. These measurements are useful for laboratory and trouble shooting classes of application.

A.1 Basic concepts in transient assessment

A very severe transient can result in a negligible overvoltage if a surge arrester installed nearby diverts its energy off line to protect the equipment, although this can cause damage to arresters. To ensure that useful information is gleaned from measurements, a technique for assessing transients and recommendations for the window width and sampling rate are given below.

A.2 Source voltage assessment

The basic reason for measuring transients is to compare measured values with those used to verify the immunity of electrical and electronic equipment connected to the distribution system.

It should be kept in mind that the transients-immunity test aims to predict the performance of electrical equipment over its normal service life. To certify an electrical appliance as acceptable for use, manufacturers employ transient generators that comply with the standards applicable to the equipment to be tested. These standards specify an open-circuit voltage Ug which decreases at the terminals of an impedance Zs at the moment the generator injects a current into the equipment under test. This impedance Zs is known as the artificial mains network or line impedance stabilization network (LISN) which is specified as a function of the range of frequencies contained in the transient, as follows:

- (0.4 W + 800 m H) for frequencies lower than 9 kHz [IEC 725]

- 50 W in parallel with (5 W + 50 m H) [CISPR 16] for frequencies from 9 kHz - 150 kHz

- 50 W in parallel with 50 m H [CISPR 16] for frequencies from 150 kHz to 30 MHz.

In immunity tests, the reproducibility of transient severity is ensured by the LISN which supports the idea of associating the measured transient current to the transient voltage drop across the LISN. The source voltage corresponds to the sum of the actual measured transient voltage and the assessed voltage drop across the LISN produced by the measured transient current. This approach has the advantage of offering a common basis for comparison by fixing the supply impedance and offers the possibility of standardizing the load impedance by connecting a non-linear load.

The LISN assessment approach allows transient severity to be assessed for any type of load. Therefore, the addition of non-linear load at the point of measurement limits the voltage scale of the instrument without affecting the of the transient severity assessment.

In summary, the LISN assessment approach gives adequate source voltage waveforms UaS, UbS, and UcS so that a transient generator could reproduce transients Ua, Ub, and Uc as recorded if connected to the same load. These voltage waveforms include the measured voltage and the low-, medium- and high-frequency voltage components Ua-LF, Ub-LF, Uc-LF, Ua-MF, Ub-MF, Uc-MF, Ua-HF, Ub-HF, Uc-HF across the impedance of the assumded system which is produced by the transient current at the PCC. Variables Ua-LF, Ub-LF, Uc-LF, Ua-MF, Ub-MF, Uc-MF, Ua-HF, Ub-HF, Uc-HF can be calculated from the measured current.

The transient voltage analysed should include the fundamental and all harmonic components of the power-system voltage. However, for classification purposes, the transient voltage should be extracted from the mains voltage.

The transient current should be filtered using a digital filter to supply the low-frequency (below 9 kHz) component Ia-LF(t), Ib-LF(t) and Ic-LF(t) and the high-frequency (above 9 kHz) component Ia-MF(t), Ib-MF(t) and Ic-MF(t). The filtered current then serves to rebuild two transient voltage waveforms using components below and above 9 kHz as needed in Equations. 1 to 5§ which estimate the voltage drop across the source impedance of the assumed system:

 

[1]

where

[2]

where

[3]

where

 

[4]

where

 

[5]

where

[6]

where

Lastly, the source voltages UaS, UbS, and UcS to be compared to the values recommended in the standards for susceptibility tests are

[7]

[8]

[9]

A.3 Window width and sampling rate

The measurement instrumentation therefore needs a four-cycle window width of recorded data so as to analyse capacitor switching transients with a frequency component below 5 kHz [IEEE 62.41]. Tests have shown that a minimum sampling rate of 20 kilosamples per second (ksamples/s)is needed to record this type of low-frequency transient which is 4 sampled values per period of 5 kHz signal. However, 4 ksamples/s sampling rate records properly most low-frequency transients which are produced by capacitor-switching transients characterised by frequency components below 1 kHz.

 

- for legal class : sampling rate should be above 36  ksamples/s

- for benchmarking class : sampling rate should be above 4 ksamples/s,.

A power distribution system comprises multiple interconnected elements. At each connection, the surge impedance changes, with the result that the transient can be reflected and increase as much as twofold at the point of reflection, becoming a local ring wave. The sampling rate for recording this type of transient should be higher than 2 megasamples per second(Msamplse/s) but IEC 816 recommends 150 mega-samples per second.

- for laboratory class: sampling rate should be above 150 000 ksamples/s

- for trouble shooting class: sampling rate should be above >2 000 ksamples/s,.

A.4 Transient overvoltage envelope

Transient  recorded waveforms do usually not contain exactly the frequency components composing the reference transient used to test equipment. However, the severity in terms of energy can be assessed by comparing the rms voltage envelope of the recorded transient to the rms voltage envelope of the reference transient.

The voltage envelope consists of a curve showing the severity of the disturbances as momentary rms voltage deviations from the declared voltage that lasts a certain period of time.

The rms voltage assessment is used to assess the rms voltage envelope for a duration exceeding a half cycle. However, the voltage envelopes of transients lasting less than a half cycle are more complex to assess and need a special assessment method.

When the supply voltage U(t) includes a short transient detected at time a , the percent voltage Vp of interval T related to the voltage envelope is given by:

%

% [10]

where:

Vp = rms voltage as a percentage of the declared voltage Vd

Vd = rms declared voltage

a = beginning of the interval assessed

T = interval assessed

U(t) = supply voltage involving a short transient.

D t = sampling interval

The aim of transient analysis is to identify a suitable time a which yields the maximum Vp calculated with Eq. 10.

A.5 Rms amplitude-duration decomposition

The following procedure is used to assess the Vp maximum values related to the interval T for all incremented a :

  1. All transients within the limit of frequency ranges specified must be detected and recorded. The suggested detection technique can be either the MAVSA technique described in the Canadian Electrical Association report 220 D 711 (see the reference in the tutorial on 3-s interval rms value assessment) for low-frequency transients or using the voltage components of frequencies above 9 kHz of amplitude exceeding 10% of the declared peak-voltage value (voltage level trigger). The slope technique can also be used. When applied to a signal sampled at least every 25 µs by a Category 1 instrument, the MAVSA technique detects transients with a frequency component below 9 kHz. However, a lower sampling interval such as 250 µs is allowed for Category 2 instruments to assess most switching transients driven by a capacitor bank, these constitute most low-frequency oscillatory transients. At least 4 cycles of signal are needed to analyse a low-frequency transient if all subsequent possible transients due to restrike between the contacts of the switching device are to be considered.
  2. A voltage-level trigger calls for a sampling rate of at least 2 Msamples per second for Category 2 instruments to assess high-frequency and impulsive transients such as those produced by lightning strikes. At least 2 ms of recorded signals are needed for analysing all possible forward-backward reflection transients but 40 ms of recorded signal, sampled at a lower rate during the medium-frequency transient are also required to provide one full cycle (used in step 8).

  3. The pre-triggering interval of 30 µs or a 8 ms signal is added before the beginning of the short transient triggered by the frequency voltage component of the signal or by the MAVSA respectively. The start of the pre-triggering interval marks the beginning of time a .
  4. A fourth-order digital high-pass 9 kHz filter used to process the transient current obtained in step 2 gives the medium-frequency transient current
    Ia-HF(t), Ib-HF(t) and Ic-HF(t).
  5. Samples of the medium-frequency current obtained in step 3 are then subtracted from the corresponding samples in step 2 to give the low-frequency currents Ia-LF(t), Ib-LF(t) and Ic-LF(t).
  6. Measured samples of the short transient are then processed using Equation 7, 8 or 9 to calculate the source voltages UaS, UbS, and UcS.
  7. Source voltages of the short transient are then processed using Equation 10 to give sets of voltage-duration values (UeS, TeS) for durations up to 5 ms. All UeS values below ISV% are set to the lowest Ue value above ISV%. The variable ISV% is calculated using the following equation:

% [11]

where:

ISV = instantaneous steady-state voltage calculated in section 6.16

Vd = rms declared voltage.

  1. Repeat step 6 moving the reference time a forward in 0.5 µs increments for medium-frequency and impulse transients and 30 µs increments for low-frequency transients until the end of the recorded signal is reached. Calculate the root mean square of voltages UeS at each half-decade of each iteration. This value in the interval between each half-decade yields a value for the factors of the rms envelope, as follows:

VHFC =

root mean square of voltages between 1 µs and 5 µs

HFC =

root mean square of voltages between 5 µs and 10 µs

HMFC =

root mean square of voltages between 10 µs and 50 µs

MFC =

root mean square of voltages between 50 µs and 100 µs

MLFC =

root mean square of voltages between 100 µs and 500 µs

LFC =

root mean square of voltages between 500 µs and 1 ms

VLFC =

root mean square of voltages between 1 ms and 5 ms

  1. A sixth-order digital high-pass 240 Hz filter used to process the transient voltage obtained in step 1 gives the transient-specific data needed for step 9.
  2. Calculate the peak voltage of each polarity and the peak-to-peak voltage of the transient alone, obtained in 8. If the absolute amplitude for a given polarity exceeds 77% of the peak-to-peak value the results in step 8 are placed in the category of impulsive transients ITV. If the test fails to classify the ITV transients, pass to step 10.  
  3. Classify the results of step 7 in the category of high-frequency oscillating transients and proceed to the final clasification if the interval measured in step 8 containing three zero crossings of the transient is less than 111 µs. A zero crossing occurs when the transient changes polarity and reaches a level exceeding 23% of the peak-to-peak value.
  4. Classify the results of step 7 in the category of low-frequency oscillating transients if the test of step 9 and 10 fails to classify the transient..

       

References

  1. Roger Bergeron, "Voltage Unbalance on Dstribution Systems - Phase I", Canadian Electrical Association, Project No. 231 D 488, Montréal, Québec, January 1989.

  1. Westinghouse Electric Corporation. "Applied Protective Relaying", Silent Sentinels publication, Newark, New Jersey.

  1. Cumming, P.G. "Protection of Induction Motors Against Unbalance Voltage Operation", IEEE-PCI, September 1983, IEEE-PIT, June 1984 and IEEE-IAS October 1984.

  1. Roger Bergeron, "A Measurement Protocol for Power Quality Coordination", CIRED 1991, paper 2.17, April 1991.

  1. IEC 27-1 (1992).- Letter Symbols To Be Used in Electrical Technology. Part 1: General.

  1. IEC 146. Parts 1 to 6 .- Semiconductors Convertors.

  1.     IEC 375 (1972).- Conventions Concerning Electric and Magnetic Circuits.
  1. Roger Bergeron, "Power Quality Measurement Protocol, CEA Guide to Performing Power Quality Surveys," CEA report 220 D 711, Canadian Electrical Association 1 Westmount Square, Suite 1600 Montréal, Québec, Canada H3Z 2P9, 1996, 216 pp.

 

 

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