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978-1-5386-5086-8/18/$31.00 ©2018 IEEE
Power Quality Indices for Electrical Power Systems
under Non-Stationary Disturbances
P. A. Karafotis, K. N. Christodoulou-Galanopoulos, D. O. Siagkas, P. S. Georgilakis
National Technical University of Athens, School of Electrical and Computer Engineering
9, Iroon Polytechniou, Athens, Greece
panoskarafo@gmail.com
Abstract: This paper presents a methodology to evaluate
power quality indices using Wavelet Packet Transform in
electrical power systems, in the presence of harmonics, under
stationary, non-stationary and short-circuit occurrence
conditions, in order to achieve efficient monitoring of power
systems. Results on several test systems and various disturbances
simulated by Matlab/Simulink demonstrate the effectiveness and
robustness of the proposed method.
I. INTRODUCTION
The term power quality (PQ) indicates the deviation of both
voltage and current from their ideal waveforms. An ideal
waveform is considered to be sinusoidal, with fixed frequency
and amplitude, any deviation from which is considered a
disturbance. With the increased use of nonlinear loads, as well
as due to time-varying single-phase and three-phase loads, the
deformation of voltage and current from their ideal waveform
has increased to a large extent. Therefore, the quantification of
these deformations, using appropriate power quality indices
(PQIs), has become a quite important issue in modern electrical
power systems and offers the opportunity of efficient
monitoring of power system quality. Total harmonic distortion
of voltage and current, distortion index of voltage and current,
as well as power factor, are worldwide established PQIs
capable of compressing raw information, usually
multidimensional in nature, into a single value [1].
Most PQIs currently used, are based on the analysis of
voltage and current waveforms in their individual harmonic
components. In order to analyze these disturbances and extract
their spectrum, Fourier Transform (FT) is widely used [2]–[3].
However, using FT, signals can be described exclusively in the
time or frequency domain, failing to provide information about
time tracing of different frequencies within the signal. Thus,
FT is no longer considered as the most suitable method for
analyzing non-stationary disturbances containing time-varying
frequency spectrum, such as short circuits. To address these
problems, as well as to improve the existing PQIs and
monitoring services, the wavelet transform (WT) is
investigated. WT provides simultaneous time-frequency
information of a signal, and as a result is more accurate in
evaluating PQIs in electrical power systems with non-
stationary disturbances [4]–[8].
In the present paper, Wavelet Packet Transform (WPT) is
proposed to evaluate the PQ performance of single-phase and
three-phase electrical power systems, operating under both
stationary and non-stationary conditions. Typical PQ
components, such as voltage, current and power, are
reformulated by WPT and the most critical PQIs are calculated.
Their values are presented and compared with their true values
and those calculated with FT, in order to validate: 1) the ability
of WPT to provide very accurate results in electrical power
systems operating under both stationary and non-stationary
conditions, 2) the advantage of WPT over FT to assess PQ
performance in electrical power systems operating under non-
stationary conditions, 3) the inability of FT to recognize short
time disturbances.
This paper is organized as follows. Section II presents the
WPT based mathematical approach to calculate PQIs. In
Section III, the test cases and scenarios considered are
described and the obtained results are presented. Conclusions
are drawn in Section IV.
II. MATHEMATICAL APPROACH
A. Wavelet Packet Transform
Using a pair of filters, a low-pass  l n and a high-pass
 h n , the initial waveform given by the matrix  0
0d k , is
analyzed into j decomposition levels. The initial matrix
 0
0d k contains 2N
samples and at each level j and node i ,
the WPT coefficients are derived from those of the previous
level, by the convolution of the coefficients of the previous
level with the low pass and the high pass filter, by the
following equations, respectively:
     2
1 2 i i
j j
n
d k l n d k n (1)
       

n
i
j
i
j nkdnhkd 21
12
(2)
where n is an internal variable of the convolution
mathematical operation. Thus, in the final decomposition level,
the signals  i
jd k contain 2 N j
WPT coefficients and a
frequency range of
2
maxf
, where maxf is the maximum
frequency of the original signal. The maximum frequency is
calculated using the sampling frequency sf of the signal,
based on the sampling theorem, by:
2
s
max
f
f  (3)
B. Voltage, Current and Power Formulation
The initial voltage and current disturbance is decomposed up
to level j , in the way that each node includes exactly an odd
harmonic order. Assuming that the WPT coefficients of each
node i at the decomposition level j are  i
jd k and  i
jc k for
voltage and current respectively, their RMS values i
jV and i
jI
at each node i are computed by:
  




12
0
2
2
1
jN
k
i
jN
i
j kdV (4)
  




12
0
2
2
1
jN
k
i
jN
i
j kcI (5)
Using the RMS values of each node i , the total RMS values
of voltage and current rmsV and rmsI are calculated by:
 
2 1 2
0


 
j
i
rms j
i
V V (6)
 
2 1 2
0


 
j
i
rms j
i
I I (7)
Active power i
jP at each node i is given by:
    
2 1
0
1
2



 
N j
i i i
j j jN
k
P d k c k (8)
while the total active power P is computed by:
2 1
0


 
j
i
j
i
P P (9)
The node zero apparent power j
0
S is given by:
0 0 0
j j jS V I (10)
while the total apparent power S is calculated by:
 rms rmsS V I (11)
C. Power Quality Indices
Using the mathematical expressions of voltage, current and
power of Section II.B, Total Harmonic Distortion of Voltage
and Current, VTHD and ITHD , respectively, are given by:
    
  
2 1 2 1 2 12 2
1 1 0
0 2 1 20
0
j j N j
N j
i i
j j
i i k
V
j
j
k
V d k
THD
V
d k


  
  


 
  

(12)
    
  
2 1 2 1 2 12 2
1 1 0
0 2 1 20
0


  
  


 
  

j j N j
N j
i i
j j
i i k
I
j
j
k
I c k
THD
I
c k
(13)
Distortion Index VDIN and IDIN is defined as the ratio of
the vector sum of the rms value of each node except node zero,
to the total rms value of the original waveform, as:
    
  
2 1 2 1 2 12 2
1 1 0
2 1 2 1 2
0 0
j j N j
j N j
i i
j j
i i k
V
irms
j
i k
V d k
DIN
V
d k


  
  
 
 
 
  
 
(14)
    
  
2 1 2 1 2 12 2
1 1 0
2 1 2 1 2
0 0


  
  
 
 
 
  
 
j j N j
j N j
i i
j j
i i k
I
irms
j
i k
I c k
DIN
I
c k
(15)
Power factor PF can be calculated by:
    
   
2 1 2 1
0 0
2 1 2 12 2
0 0
1
2
j N j
j j
i i
j jN
i k
i i
j j
i i
d k c k
P
PF
S
V I

 
 
 
 
 
 
 
(16)
while node zero power factor NZPF is defined as the ratio of
the active power of node zero to the apparent power of node
zero:
0
0

j
NZ
j
P
PF
S
(17)
III. CASE STUDIES AND RESULTS
The proposed methodology has been tested in three different
case studies, including representative scenarios, in order to
examine several possible operating conditions of electrical
power systems, as shown in Table I.
TABLE I
CASES STUDIES AND SCENARIOS CONSIDERED
Case
study
Scenario Input source Input waveform
C1
S1 time domain equation stationary
S2 time domain equation non-stationary
C2
S1 single-phase power system stationary
S2 single-phase power system non-stationary
S3 single-phase power system
non-stationary
(short-circuit)
C3
S1 three-phase power system stationary
S2 three-phase power system non-stationary
S3 three-phase power system
non-stationary
(short-circuit)
A. Case Study C1
In the first case study (C1), two scenarios (S1 and S2) are
considered, in which the time domain equation of the
waveforms are known. In S1, voltage and current waveforms
are stationary, while in S2, non-stationary. In both S1 and S2,
the fundamental frequency of the waveforms is 50 Hz, the
observation period is 0.2 s and the waveforms are decomposed
up to the 4th level, so that each frequency band corresponds to
an odd harmonic component.
In S1, stationary voltage and current waveforms are
simulated, containing 1st
, 3rd
, 5th
, 7th
, 9th
, 11th
, and 13th
harmonic component, as follows:
   
   
   
 
( ) 2 230sin 2 46sin 2 3 135
46sin 2 5 150 23sin 2 7 140
18,4sin 2 9 40 23sin 2 11 15
23sin 2 13 150
     
     
     
 
v t ft ft
ft ft
ft ft
ft
 
 
 

(18)
   
   
   
 
( ) 2 10sin 2 10 sin 2 3 150
0,8sin 2 5 135 0,8sin 2 7 22,5
0,9sin 2 9 20 0,7sin 2 11 45
0,8sin 2 13 120
       
     
     
 
i t ft ft
ft ft
ft ft
ft
 
 
 

(19)
In S2, the amplitude of the fundamental component of
voltage waveform is 240 2 for up to 0.08t  s and then drops
to 72 2 until the end of the simulation (0.2 s). Apart from the
fundamental component, voltage waveform also contains 5th
and 7th
harmonic components with amplitudes 60 2 and
40 2 respectively, throughout the observation period. The
current waveform contains the fundamental component with an
amplitude of 50 2 up to 0.08t  s, 15 2 for
 0.08,0.13t  and once again 50 2 until the end of the
simulation. It also contains 3rd
, 5th
and 7th
harmonic
components up to 0.13t  s, with amplitudes 12.5 2 , 10 2
and 7.5 2 , respectively, and then they drop to zero.
The true values of PQIs for both S1 and S2 of C1, as well as
the values calculated by WPT and FT are presented in Table II.
The percentage difference between true values and the values
calculated by WPT and FT are presented in Table III.
TABLE II
POWER QUALITY INDICES FOR CASE STUDY C1
PQIs
S1 S2
True
values WPT FT
True
values WPT FT
VTHD 0.3412 0.3429 0.3435 0.4461 0.4477 0.5237
ITHD 0.2054 0.2070 0.2079 0.3243 0.3262 0.4113
VDIN 0.3229 0.3244 0.3248 0.4074 0.4086 0.4640
IDIN 0.2012 0.2027 0.2035 0.3085 0.3101 0.3804
NZPF 0.9848 0.9848 0.8750 0.8792
PF 0.9565 0.9565 0.8320 0.8320
B. Case Study C2
In the second case study (C2), a single-phase circuit is
considered, simulated by Matlab/Simulink, including three
different loading scenarios (S1, S2 and S3). The circuit
consists of a 24V DC voltage source, a DC/AC inverter
controlled by SPWM control technique, and a transformer to
increase the voltage to 230 V, as shown in Fig. 1.
TABLE III
PERCENTAGE DIFFERENCE OF POWER QUALITY INDICES FOR CASE STUDY C1
PQIs
S1 S2
WPT FT WPT FT
VTHD 0.50 % 0.67 % 0.36 % 17.40 %
ITHD 0.78 % 1.20 % 0.59 % 26.83 %
VDIN 0.46 % 0.59 % 0.29 % 13.80 %
IDIN 0.75 % 1.14 % 0.52 % 23.31 %
In S1, a load of 9 kW is connected throughout the whole
simulation period, thus voltage and current waveforms are
stationary. In S2, two loads are connected to the circuit, a load
of 8 kW, and a load of 1.5 kW and 1.5 kVar, for different
amount of time, in order to examine how FT and WPT respond
under non-stationary conditions. The first load is connected to
the circuit during    0,0.206 0.266,0.4t   , while the second
during  0.16,0.4t  . In S3, the same loads of second scenario
are connected to the circuit, however, a short-circuit is added
for a brief amount of time during  0.320,0.322t  . The
values of PQIs calculated by WPT and FT for the three
scenarios (S1, S2 and S3) of C2, as well as the percentage
difference between WPT and FT, are presented in Table IV.
Figure 1. Single-phase power system for case study C2
TABLE IV
POWER QUALITY INDICES FOR CASE STUDY C2
Scenario PQIs WPT FT Difference %
S1
VTHD 0.3026 0.3026 0.00
ITHD 0.3026 0.3026 0.00
S2
VTHD 0.3639 0.3321 9.58
ITHD 0.2978 0.2825 5.42
S3
VTHD 0.3683 0.3316 11.08
ITHD 0.3316 0.2838 16.84
C. Case Study C3
The third case study (C3) includes a symmetrical three-phase
circuit, also simulated by Matlab/Simulink, examining three
loading scenarios (S1, S2 and S3) similar to those in C2. As
shown in Fig. 2, the circuit consists of a 48 V DC voltage
source, a three-phase bridge inverter controlled by SPWM
control technique, and a step-up transformer.
In S1, a symmetric three-phase load of 15 kW is connected
to a grounded earth connection throughout the observation
period. In S2, a three-phase load of 15 kW, during
   0,0.8 0.104,0.24t   , and a symmetrical three-phase load
of 10 kW and 6.2 kVar during  0.12,0.24t  are connected to
the circuit. In S3, the same loads, as in S2, are connected to the
circuit, but also a symmetrical three-phase short circuit during
 0.18,0.1824t  is added.
Figure 2. Three-phase power system for case study C3
The values of PQIs calculated by WPT and FT for the three
scenarios (S1, S2 and S3) of C3, as well as the percentage
difference between WPT and FT, are presented in Table V.
TABLE V
POWER QUALITY INDICES FOR CASE STUDY C3
Scenario PQIs WPT FT Difference %
S1
VTHD 0.2452 0.2440 0.49
ITHD 0.2452 0.2440 0.49
S2
VTHD 0.3770 0.3304 14.10
ITHD 0.2385 0.2376 0.38
S3
VTHD 0.4329 0.3397 27.44
ITHD 0.3460 0.2425 42.68
IV. CONCLUSION
The proposed method for PQIs evaluation using WPT is
tested on Matlab/Simulink simulated power systems and
disturbances, both stationary and non-stationary, and the
results obtained are compared with their true values and those
by FT. The results validate that WPT is more suitable method
than FT in evaluating power quality in electrical power
systems operating under non-stationary conditions. Specifically,
the following conclusions have been drawn from the above
three case studies of Section III:
 In C1, it is verified that PQIs are accurately computed by
the proposed WPT method, since their values are
compared with their true ones, with the percentage
difference being negligible and smaller than the difference
between FT and true values.
 In S1, for both C2 and C3, where voltage and current
waveforms are stationary, WPT and FT provide almost the
same values for all PQIs.
 In S2, for both C2 and C3, where the loads are not
constant, therefore voltage and current waveforms are
non-stationary, WPT and FT provide quite different
results, due to the disadvantage of FT to deal with time-
varying loads.
 In S3, for both C2 and C3, with the addition of a transient
phenomenon lasting for a very short period of time (short-
circuit), the values of the PQIs computed by FT do not
really change in comparison with S2, while by WPT are
increased considerably. This result indicates that FT is not
able to recognize short time highly non-stationary
phenomena, like short-circuits, in contrast with WPT,
where the values of PQIs changed significantly.
The proposed method can be integrated in modern
distribution management systems, providing the operators the
opportunity of efficient monitoring of power system quality.
REFERENCES
[1] M. S. Kandil, S. A. Farghal, and A. Elmitwally, “Refined power quality
indices,” IEΕE Proc. Gener. Transm. Distrib., vol. 148, no. 6, pp.
590596, Nov. 2001.
[2] Electromagnetic compatibility (EMC) - Part 3-6: Limits - assessment of
emission limits for the connection of distorting installations to MV, HV
and EHV power systems, IEC TR 61000-3-6, 2008.
[3] Definitions for the measurement of electric quantities under sinusoidal,
non-sinusoidal, balanced, or unbalanced conditions, IEEE Standard
1459-2010, Mar. 2010.
[4] C. A. Naik and P. Kundu, “Power quality index based on discrete wavelet
transform,” Int. J. Electr. Power Energy Syst., vol. 53, pp. 9941002,
Dec. 2013.
[5] K. Thirumala, A. C. Umarikar, and T. Jain, “Estimation of single-phase
and three-phase power-quality indices using empirical wavelet
transform,” IEEE Trans. Power Del., vol. 30, pp. 445–454, Feb. 2015.
[6] W. G. Morsi and M. E. El-Hawary, “Reformulating power components
definitions contained in the IEEE Standard 1459-2000 using discrete
wavelet transform,” IEEE Trans. Power Del., vol. 22, pp. 1910–1916,
Jul. 2007.
[7] E. Y. Hamid, R. Maridiana, and Z. I. Kawasaki, “Method for RMS and
power measurements based on the wavelet packet transform,” IEEE
Proc. Sci. Meas. Technol., vol. 149, no. 2, pp. 6066, Mar. 2002.
[8] W. G. Morsi and M. E. El-Hawary, “Novel power quality indices based
on wavelet packet transform for non-stationary sinusoidal and non-
sinusoidal disturbances,” Electr. Power Syst. Res., vol. 80, no. 7, pp.
753759, Jul. 2010.

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Power Quality Indices for Electrical Power Systems under Non-Stationary Disturbances

  • 1. 978-1-5386-5086-8/18/$31.00 ©2018 IEEE Power Quality Indices for Electrical Power Systems under Non-Stationary Disturbances P. A. Karafotis, K. N. Christodoulou-Galanopoulos, D. O. Siagkas, P. S. Georgilakis National Technical University of Athens, School of Electrical and Computer Engineering 9, Iroon Polytechniou, Athens, Greece panoskarafo@gmail.com Abstract: This paper presents a methodology to evaluate power quality indices using Wavelet Packet Transform in electrical power systems, in the presence of harmonics, under stationary, non-stationary and short-circuit occurrence conditions, in order to achieve efficient monitoring of power systems. Results on several test systems and various disturbances simulated by Matlab/Simulink demonstrate the effectiveness and robustness of the proposed method. I. INTRODUCTION The term power quality (PQ) indicates the deviation of both voltage and current from their ideal waveforms. An ideal waveform is considered to be sinusoidal, with fixed frequency and amplitude, any deviation from which is considered a disturbance. With the increased use of nonlinear loads, as well as due to time-varying single-phase and three-phase loads, the deformation of voltage and current from their ideal waveform has increased to a large extent. Therefore, the quantification of these deformations, using appropriate power quality indices (PQIs), has become a quite important issue in modern electrical power systems and offers the opportunity of efficient monitoring of power system quality. Total harmonic distortion of voltage and current, distortion index of voltage and current, as well as power factor, are worldwide established PQIs capable of compressing raw information, usually multidimensional in nature, into a single value [1]. Most PQIs currently used, are based on the analysis of voltage and current waveforms in their individual harmonic components. In order to analyze these disturbances and extract their spectrum, Fourier Transform (FT) is widely used [2]–[3]. However, using FT, signals can be described exclusively in the time or frequency domain, failing to provide information about time tracing of different frequencies within the signal. Thus, FT is no longer considered as the most suitable method for analyzing non-stationary disturbances containing time-varying frequency spectrum, such as short circuits. To address these problems, as well as to improve the existing PQIs and monitoring services, the wavelet transform (WT) is investigated. WT provides simultaneous time-frequency information of a signal, and as a result is more accurate in evaluating PQIs in electrical power systems with non- stationary disturbances [4]–[8]. In the present paper, Wavelet Packet Transform (WPT) is proposed to evaluate the PQ performance of single-phase and three-phase electrical power systems, operating under both stationary and non-stationary conditions. Typical PQ components, such as voltage, current and power, are reformulated by WPT and the most critical PQIs are calculated. Their values are presented and compared with their true values and those calculated with FT, in order to validate: 1) the ability of WPT to provide very accurate results in electrical power systems operating under both stationary and non-stationary conditions, 2) the advantage of WPT over FT to assess PQ performance in electrical power systems operating under non- stationary conditions, 3) the inability of FT to recognize short time disturbances. This paper is organized as follows. Section II presents the WPT based mathematical approach to calculate PQIs. In Section III, the test cases and scenarios considered are described and the obtained results are presented. Conclusions are drawn in Section IV. II. MATHEMATICAL APPROACH A. Wavelet Packet Transform Using a pair of filters, a low-pass  l n and a high-pass  h n , the initial waveform given by the matrix  0 0d k , is analyzed into j decomposition levels. The initial matrix  0 0d k contains 2N samples and at each level j and node i , the WPT coefficients are derived from those of the previous level, by the convolution of the coefficients of the previous level with the low pass and the high pass filter, by the following equations, respectively:      2 1 2 i i j j n d k l n d k n (1)          n i j i j nkdnhkd 21 12 (2) where n is an internal variable of the convolution mathematical operation. Thus, in the final decomposition level, the signals  i jd k contain 2 N j WPT coefficients and a frequency range of 2 maxf , where maxf is the maximum frequency of the original signal. The maximum frequency is calculated using the sampling frequency sf of the signal, based on the sampling theorem, by: 2 s max f f  (3)
  • 2. B. Voltage, Current and Power Formulation The initial voltage and current disturbance is decomposed up to level j , in the way that each node includes exactly an odd harmonic order. Assuming that the WPT coefficients of each node i at the decomposition level j are  i jd k and  i jc k for voltage and current respectively, their RMS values i jV and i jI at each node i are computed by:        12 0 2 2 1 jN k i jN i j kdV (4)        12 0 2 2 1 jN k i jN i j kcI (5) Using the RMS values of each node i , the total RMS values of voltage and current rmsV and rmsI are calculated by:   2 1 2 0     j i rms j i V V (6)   2 1 2 0     j i rms j i I I (7) Active power i jP at each node i is given by:      2 1 0 1 2      N j i i i j j jN k P d k c k (8) while the total active power P is computed by: 2 1 0     j i j i P P (9) The node zero apparent power j 0 S is given by: 0 0 0 j j jS V I (10) while the total apparent power S is calculated by:  rms rmsS V I (11) C. Power Quality Indices Using the mathematical expressions of voltage, current and power of Section II.B, Total Harmonic Distortion of Voltage and Current, VTHD and ITHD , respectively, are given by:         2 1 2 1 2 12 2 1 1 0 0 2 1 20 0 j j N j N j i i j j i i k V j j k V d k THD V d k                 (12)         2 1 2 1 2 12 2 1 1 0 0 2 1 20 0                 j j N j N j i i j j i i k I j j k I c k THD I c k (13) Distortion Index VDIN and IDIN is defined as the ratio of the vector sum of the rms value of each node except node zero, to the total rms value of the original waveform, as:         2 1 2 1 2 12 2 1 1 0 2 1 2 1 2 0 0 j j N j j N j i i j j i i k V irms j i k V d k DIN V d k                    (14)         2 1 2 1 2 12 2 1 1 0 2 1 2 1 2 0 0                    j j N j j N j i i j j i i k I irms j i k I c k DIN I c k (15) Power factor PF can be calculated by:          2 1 2 1 0 0 2 1 2 12 2 0 0 1 2 j N j j j i i j jN i k i i j j i i d k c k P PF S V I                (16) while node zero power factor NZPF is defined as the ratio of the active power of node zero to the apparent power of node zero: 0 0  j NZ j P PF S (17) III. CASE STUDIES AND RESULTS The proposed methodology has been tested in three different case studies, including representative scenarios, in order to examine several possible operating conditions of electrical power systems, as shown in Table I. TABLE I CASES STUDIES AND SCENARIOS CONSIDERED Case study Scenario Input source Input waveform C1 S1 time domain equation stationary S2 time domain equation non-stationary C2 S1 single-phase power system stationary S2 single-phase power system non-stationary S3 single-phase power system non-stationary (short-circuit) C3 S1 three-phase power system stationary S2 three-phase power system non-stationary S3 three-phase power system non-stationary (short-circuit) A. Case Study C1 In the first case study (C1), two scenarios (S1 and S2) are considered, in which the time domain equation of the waveforms are known. In S1, voltage and current waveforms are stationary, while in S2, non-stationary. In both S1 and S2, the fundamental frequency of the waveforms is 50 Hz, the observation period is 0.2 s and the waveforms are decomposed up to the 4th level, so that each frequency band corresponds to an odd harmonic component.
  • 3. In S1, stationary voltage and current waveforms are simulated, containing 1st , 3rd , 5th , 7th , 9th , 11th , and 13th harmonic component, as follows:               ( ) 2 230sin 2 46sin 2 3 135 46sin 2 5 150 23sin 2 7 140 18,4sin 2 9 40 23sin 2 11 15 23sin 2 13 150                     v t ft ft ft ft ft ft ft        (18)               ( ) 2 10sin 2 10 sin 2 3 150 0,8sin 2 5 135 0,8sin 2 7 22,5 0,9sin 2 9 20 0,7sin 2 11 45 0,8sin 2 13 120                       i t ft ft ft ft ft ft ft        (19) In S2, the amplitude of the fundamental component of voltage waveform is 240 2 for up to 0.08t  s and then drops to 72 2 until the end of the simulation (0.2 s). Apart from the fundamental component, voltage waveform also contains 5th and 7th harmonic components with amplitudes 60 2 and 40 2 respectively, throughout the observation period. The current waveform contains the fundamental component with an amplitude of 50 2 up to 0.08t  s, 15 2 for  0.08,0.13t  and once again 50 2 until the end of the simulation. It also contains 3rd , 5th and 7th harmonic components up to 0.13t  s, with amplitudes 12.5 2 , 10 2 and 7.5 2 , respectively, and then they drop to zero. The true values of PQIs for both S1 and S2 of C1, as well as the values calculated by WPT and FT are presented in Table II. The percentage difference between true values and the values calculated by WPT and FT are presented in Table III. TABLE II POWER QUALITY INDICES FOR CASE STUDY C1 PQIs S1 S2 True values WPT FT True values WPT FT VTHD 0.3412 0.3429 0.3435 0.4461 0.4477 0.5237 ITHD 0.2054 0.2070 0.2079 0.3243 0.3262 0.4113 VDIN 0.3229 0.3244 0.3248 0.4074 0.4086 0.4640 IDIN 0.2012 0.2027 0.2035 0.3085 0.3101 0.3804 NZPF 0.9848 0.9848 0.8750 0.8792 PF 0.9565 0.9565 0.8320 0.8320 B. Case Study C2 In the second case study (C2), a single-phase circuit is considered, simulated by Matlab/Simulink, including three different loading scenarios (S1, S2 and S3). The circuit consists of a 24V DC voltage source, a DC/AC inverter controlled by SPWM control technique, and a transformer to increase the voltage to 230 V, as shown in Fig. 1. TABLE III PERCENTAGE DIFFERENCE OF POWER QUALITY INDICES FOR CASE STUDY C1 PQIs S1 S2 WPT FT WPT FT VTHD 0.50 % 0.67 % 0.36 % 17.40 % ITHD 0.78 % 1.20 % 0.59 % 26.83 % VDIN 0.46 % 0.59 % 0.29 % 13.80 % IDIN 0.75 % 1.14 % 0.52 % 23.31 % In S1, a load of 9 kW is connected throughout the whole simulation period, thus voltage and current waveforms are stationary. In S2, two loads are connected to the circuit, a load of 8 kW, and a load of 1.5 kW and 1.5 kVar, for different amount of time, in order to examine how FT and WPT respond under non-stationary conditions. The first load is connected to the circuit during    0,0.206 0.266,0.4t   , while the second during  0.16,0.4t  . In S3, the same loads of second scenario are connected to the circuit, however, a short-circuit is added for a brief amount of time during  0.320,0.322t  . The values of PQIs calculated by WPT and FT for the three scenarios (S1, S2 and S3) of C2, as well as the percentage difference between WPT and FT, are presented in Table IV. Figure 1. Single-phase power system for case study C2 TABLE IV POWER QUALITY INDICES FOR CASE STUDY C2 Scenario PQIs WPT FT Difference % S1 VTHD 0.3026 0.3026 0.00 ITHD 0.3026 0.3026 0.00 S2 VTHD 0.3639 0.3321 9.58 ITHD 0.2978 0.2825 5.42 S3 VTHD 0.3683 0.3316 11.08 ITHD 0.3316 0.2838 16.84
  • 4. C. Case Study C3 The third case study (C3) includes a symmetrical three-phase circuit, also simulated by Matlab/Simulink, examining three loading scenarios (S1, S2 and S3) similar to those in C2. As shown in Fig. 2, the circuit consists of a 48 V DC voltage source, a three-phase bridge inverter controlled by SPWM control technique, and a step-up transformer. In S1, a symmetric three-phase load of 15 kW is connected to a grounded earth connection throughout the observation period. In S2, a three-phase load of 15 kW, during    0,0.8 0.104,0.24t   , and a symmetrical three-phase load of 10 kW and 6.2 kVar during  0.12,0.24t  are connected to the circuit. In S3, the same loads, as in S2, are connected to the circuit, but also a symmetrical three-phase short circuit during  0.18,0.1824t  is added. Figure 2. Three-phase power system for case study C3 The values of PQIs calculated by WPT and FT for the three scenarios (S1, S2 and S3) of C3, as well as the percentage difference between WPT and FT, are presented in Table V. TABLE V POWER QUALITY INDICES FOR CASE STUDY C3 Scenario PQIs WPT FT Difference % S1 VTHD 0.2452 0.2440 0.49 ITHD 0.2452 0.2440 0.49 S2 VTHD 0.3770 0.3304 14.10 ITHD 0.2385 0.2376 0.38 S3 VTHD 0.4329 0.3397 27.44 ITHD 0.3460 0.2425 42.68 IV. CONCLUSION The proposed method for PQIs evaluation using WPT is tested on Matlab/Simulink simulated power systems and disturbances, both stationary and non-stationary, and the results obtained are compared with their true values and those by FT. The results validate that WPT is more suitable method than FT in evaluating power quality in electrical power systems operating under non-stationary conditions. Specifically, the following conclusions have been drawn from the above three case studies of Section III:  In C1, it is verified that PQIs are accurately computed by the proposed WPT method, since their values are compared with their true ones, with the percentage difference being negligible and smaller than the difference between FT and true values.  In S1, for both C2 and C3, where voltage and current waveforms are stationary, WPT and FT provide almost the same values for all PQIs.  In S2, for both C2 and C3, where the loads are not constant, therefore voltage and current waveforms are non-stationary, WPT and FT provide quite different results, due to the disadvantage of FT to deal with time- varying loads.  In S3, for both C2 and C3, with the addition of a transient phenomenon lasting for a very short period of time (short- circuit), the values of the PQIs computed by FT do not really change in comparison with S2, while by WPT are increased considerably. This result indicates that FT is not able to recognize short time highly non-stationary phenomena, like short-circuits, in contrast with WPT, where the values of PQIs changed significantly. The proposed method can be integrated in modern distribution management systems, providing the operators the opportunity of efficient monitoring of power system quality. REFERENCES [1] M. S. Kandil, S. A. Farghal, and A. Elmitwally, “Refined power quality indices,” IEΕE Proc. Gener. Transm. Distrib., vol. 148, no. 6, pp. 590596, Nov. 2001. [2] Electromagnetic compatibility (EMC) - Part 3-6: Limits - assessment of emission limits for the connection of distorting installations to MV, HV and EHV power systems, IEC TR 61000-3-6, 2008. [3] Definitions for the measurement of electric quantities under sinusoidal, non-sinusoidal, balanced, or unbalanced conditions, IEEE Standard 1459-2010, Mar. 2010. [4] C. A. Naik and P. Kundu, “Power quality index based on discrete wavelet transform,” Int. J. Electr. Power Energy Syst., vol. 53, pp. 9941002, Dec. 2013. [5] K. Thirumala, A. C. Umarikar, and T. Jain, “Estimation of single-phase and three-phase power-quality indices using empirical wavelet transform,” IEEE Trans. Power Del., vol. 30, pp. 445–454, Feb. 2015. [6] W. G. Morsi and M. E. El-Hawary, “Reformulating power components definitions contained in the IEEE Standard 1459-2000 using discrete wavelet transform,” IEEE Trans. Power Del., vol. 22, pp. 1910–1916, Jul. 2007. [7] E. Y. Hamid, R. Maridiana, and Z. I. Kawasaki, “Method for RMS and power measurements based on the wavelet packet transform,” IEEE Proc. Sci. Meas. Technol., vol. 149, no. 2, pp. 6066, Mar. 2002. [8] W. G. Morsi and M. E. El-Hawary, “Novel power quality indices based on wavelet packet transform for non-stationary sinusoidal and non- sinusoidal disturbances,” Electr. Power Syst. Res., vol. 80, no. 7, pp. 753759, Jul. 2010.