Partial Discharge Source Classification and De-noising in Rotating Machines 93
Using Discrete Wavelet Transform and Directional Coupling Capacitor
Copyright © 2009 SciRes JEMAA
these machines, there are different kinds of noise and
interference signals that make measurements unreliable.
Therefore, a method is needed to separate PD from these
signals. The method this paper follows is based on DWT
which is a time-frequency transform. As known, PD is a
non-stationary signal [9]. So, conventional transforms
such as Fourier Transform (FT) may not be used to ana-
lyze spectral specifications of PD as they do not distin-
guish short-term and long-term frequency components.
But DWT considers time events of the signal. Thus, it is
capable of interpreting short-time PD pulses. Next sec-
tion discusses PD de-noising using DWT.
3. PD De-Noising Using DWT
Wavelets have very attractive features which cause them
to be used in miscellaneous applications [10]. One of the
methods which works based on these features is decom-
posing and reconstructing signals using QMF2 filters.
Reference [2] is a good context to understand how DWT
decomposition using QMF filters works. But here the
focus is on applying this technique to develop the method.
In general, DWT decomposes a signal to its basic fre-
quency components as shown in Figure 1.
Recorded signal from sensors includes both PD and
noise. It is known that noise has a stochastic nature. So, it
is expected that its energy3 is divided equally between
filter bands. But PD’s energy is mostly concentrated in a
few bands [9]. Energy of the coefficients is a reliable cri-
terion to separate bands which may contain PD more than
noise. Author’s experience showed that using 2nd order
Daubechies (db2) mother wavelet [9], more than 80% of
PD signal’s energy is gathered in one of the detail coeffi-
cients (cDs) of DWT. This is a useful result which could
be considered to determine global threshold and finally
separate PD from noise. Energy distribution of a sample is
shown in Figure 2. As it is seen cD6 (detail coefficient of
6th decomposition level) includes most of PD’s energy.
Figure 1. The tree structure of the DWT [11]; cDn is the
detail .coefficient of nth decomposition level
Figure 2. Energy distribution of the signal on each level,
using db 2
Using mentioned method, thresholds are calculated (in
fact, we train the system.). The method we calculate a
threshold is called soft-thresholding and is discussed in [9].
Then decomposing is repeated and calculated thresholds
are exerted to make weak samples of the coefficients zero.
Weak samples are supposed to be related to noise com-
ponents. Figure 3 shows the reconstructed signal using
soft-thresholding in comparison with original noise-pol-
luted PD signal.
4. A Modification to the PD De-Noising
Method
The method introduced so far, suffers from a defect in
recognizing PD sources. There are four types of signals
that may reach PD-Analyzer (PDA) equipment:
1) Internal PD (i.e. PD pulses originating from rotat-
ing machine)
2) External PD (i.e. PD pulses originating from bus bar)
3) Internal noise (i.e. noise originating from other
sources except discharges)
4) External noise (i.e. noise originating from external
agents including interferences caused by communication
systems or PDA itself)
The problem of the mentioned method (and generally
pattern-based methods) encounter is that it cannot distin-
guish external PDs from internal PDs because it works
based on pulse shape and is not dependant on the direc-
tion PD comes from.
Hence, a technique is needed to separate internal and
external PD pulses. The method used to amend the ap-
proach works based on utilizing directional couplers [10].
Figure 4 shows the overall system measuring PD by this
technique. This method (called Time-Of-Arrival) was
initially used in an analogue system to separate internal
and external PD [7]. But a major disadvantage of the
analogue system is that one should design a system which
works in frequencies upper than 50 MHz [12] because it
does not utilize any de-noising technique. Therefore,
noise eliminating is done with high-pass filtering because
there is no noise or interference in this system at those
frequencies.
2Quadrature Mirror Filter
3Energy definition and formulation of calculating coefficients’ energy
is introduced in [11].