gujarat technological university · 2018-07-05 · are multiple non-idealities in the pcc voltage,...
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INVESTIGATION INTO POWER QUALITY ISSUES AND
HARMONIC MITIGATION IN MODERN POWER SYSTEMS
A
A Synopsis submitted to Gujarat Technological University
in
Electrical Engineering
by
PATIL KALPESHKMAR ROHITBHAI
119997109007
under supervision of
Dr. Hiren H. Patel
GUJARAT TECHNOLOGICAL UNIVERSITY
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1. Abstract
Over the last couple of decade electrical power utility has observed a rapid change in electrical power
generation, transmission, as well as distribution sector. It has resulted mainly due to the deregulation and
restructuring process, advancement in technology and increased concern about the environmental
impacts.
The power generation is no longer restricted to centralized power plants, but allows energy generation
from distributed energy resources (DERs) or distributed generators (DGs). Unlike the centralized
converters that are connected directly to the utility, the DRs usually require some kind of power
electronic converters for grid interface. Various power electronic converters (often referred as FACTS
devices) with faster and sophisticated control, are also incorporated in the system to improve the
transmission and distribution capabilities and to improve the stability of the electrical power system. Not
only the utility, but the domestic and industrial consumers have also seen the proliferation of power
electronic converter to satisfy the requirements of precise control, increased efficiency and compulsion to
meet the statute/regulations set by the regulatory bodies.
These power electronic converters, which are intended to improve the capability of the system or load,
also introduce certain challenges in their designing, commissioning, operation and control; otherwise they
may degrade the performance of the network or the connected system. With increase in the penetration
level (number and size) of the converters in the existing network, the gravity of the issues presented by
these converters increase. These issues include proper synchronization, power flow control, injection of
harmonics and/or imbalance, voltage and frequency instability, resonance, change in the network
impedance, reverse power flow etc. Hence, it is must to devise a proper control scheme for the converters
to keep the undesired effect to the minimum.
One of the critical aspects in achieving the precise operation and control of the converters is the proper
synchronization of the converters with the utility. This requires the proper estimation of the phase,
frequency and magnitude of the voltage/current at the Point of Common Coupling (PCC). However, there
are multiple non-idealities in the PCC voltage, especially in the modern power system characterized by
non-linear loads and power converter based DGs. This leads to inaccurate estimation of phase and
magnitude of voltage/current, which finally affects the performance of the converters. This further inserts
harmonics and/or imbalance in the system deteriorating the power quality of the voltage/currents at the
PCC and the connected system.
The research is aimed to investigate performance of various phase/frequency estimation techniques
under various non-ideal conditions like voltage imbalance, harmonics, dc-offset etc. It is observed that
most of the methods are not capable of estimating the frequency when the grid signals are characterized
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by dc-offset. A frequency estimation technique named modified dual second order generalized
(MDSOGI) is presented which precisely estimates the frequency under all the non-ideal conditions. The
results are validated experimentally. The scheme is further integrated with the instantaneous reactive
power theory to develop a control scheme for a shunt active power filter capable of working under such
conditions. The experimental prototype is developed to signify the improved performance.
2. Brief description on the state of the art of the research topic
The environmental concern is rapidly replacing the fossil fuels based electricity generation by the
renewable energy sources i.e. wind, solar, fuel cell etc. based electricity generation. Hence, the modern
power plant is characterized by the presence of large number of power electronics converter based
distributed generation along-with traditional power plants. Almost all these power electronics converters
are committed to provide a controlled and high quality power exchange to the utility or local linear/non-
linear loads connected at the point of common coupling (PCC). Besides the power converters used for
DGs, power electronic converters are also incorporated into the system to improve the systems
performance. The power converters commonly referred as FACTS devices (name derived from flexible
AC transmission systems) are quite popular for reactive power compensation, improving static and
dynamic stability, imbalance mitigation, congestion management etc [1].
The power converters are even utilized for loads like electrical drives, uninterruptible power supply,
electrical heating and furnaces, lightings, chargers etc. These power electronic converters based load
introduce harmonics into the system causing the degradation of the power quality. The major contributor
to the power quality deterioration is the uncontrolled diode bridge rectifiers as they introduces low order
5th
and 7th
harmonics with significant amplitude. Traditionally, passive LC filters [2] were used to limit
the injection of harmonics into the utility. These filters are now replaced by the advanced power
electronics compensator known as active power filters in the modern electrical power system [3-5]. Out
of the various active power filter configurations (series, shunt and hybrid), shunt active power filter
(SAPF) is quite popular to remove harmonics locally at the load side making the utility free of harmonics
[6-11]. Unlike passive LC filters, which are simple in design, cheap, large and heavy, tuned to particular
frequency [5]; the APFs are complex and costly; however, relatively smaller, fast, free from problem of
resonance, and adaptive in nature and hence, can compensate various harmonics of different types of non-
linear loads. The performance of the SAPF is greatly dependent on how precisely the reference
compensating current is computed. The task of generating this reference compensation current is
challenging, especially when the system operates in a weak grid or micro-grid, which is very likely to
have distorted supply voltage, harmonics, imbalance in three-phase load, imbalance in supply voltage etc
[12-15]. Under such case for computing reference compensation current, it is must to accurately compute
the fundamental positive sequence components (PSCs) of grid voltage. The accuracy of the fundamental
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PSCs depends on the accurate information derived about the phase, frequency and amplitude of grid
voltage. It is also termed as the grid synchronization.
Just like active filters, all other grid-connected power electronic converters, irrespective of the
application, require proper synchronization with the grid. They also demand the correct information of
the phase, frequency and amplitude of the grid voltage for their proper operation. Otherwise instead of
improving the performance of the utility or load, they may affect the system adversely.
Various grid synchronization techniques or the phase angle estimation have been reported. These
approaches can be broadly categorized into frequency and time domain (FD and TD) techniques. The FD
techniques based on digital Fourier transform are complex to implement, require more memory and
increase in the computational burden under distorted grid signal [16]. Hence, TD approach based on
phase-locked loop (PLL) which has advantages like simplicity, better dynamic response, low sensitivity
to the variations and distortion in grid voltage etc. is preferred. Further, it has higher accuracy and is
relatively more stable and reliable. The PLL comprises of the phase detector (PD) block, filter and a
voltage controlled oscillator (VCO). The gain of VCO, whose output signal is synchronized (in terms of
phase and frequency) with the input reference signal, depends on the output of PD. The classification of
PLL based on various PD is reported and their performance is evaluated under the different grid severity
for a single-phase system [17]. The three-phase conventional PLL based on the synchronous reference
frame (SRF) have superior performance in the balanced grid voltage signal. But, it gives the oscillatory
response for the estimated fundamental frequency, if measured grid voltage signal is unbalanced or
distorted [18]. The poor performance of the conventional PLL was improved by the technique reported in
[19], which employs decoupled double synchronous reference frame PLL (DDSRF-PLL). The DDSRF-
PLL decouples the fundamental positive and negative sequence components to estimate the frequency. It
results into accurate estimation in case of unbalanced grid voltage signal. However, performance
deteriorates when grid signal is distorted. The PD structure based on generalized integrator (GI) is an
attractive solution to accurately estimate phase/frequency. However, in case of non-sinusoidal input
signals and varying frequency conditions it results into erroneous performance [20-21]. Unlike it, the
second-order GI based PLL (SOGI-PLL) shows accurate performance with the distorted input signals and
is even suitable for variable frequency applications. To compute the frequency, the SOGI-PLL
continuously utilizes the estimated frequency as a feedback for SOGI block, Unlike it, the frequency-
locked loop (FLL) adaptively obtains the frequency information avoiding the need of PLL. It further
improves the response [22-23]. The performance can further be improved by employing two SOGI-FLL
(DSOGI-FLL), resulting into better transient response and stability in the presence of grid abnormalities
[17]. However, even with DSOGI-FLL the frequency estimation is erroneous when the input signal bears
a dc-offset [24-30]. Modified SOGI-FLL structure known as modified adaptive notch filter (ANF) is
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reported to tackle the issue of dc-offset in estimation of frequency for single phase systems. Three such
ANFs are required for three-phase systems [26].
Apart from these disturbances, presence of dc component affects the performance of synchronization
schemes or phase angle estimation. The probable source of dc component can be the measurement errors,
conversion errors resulting through the data converters, inaccurate signal conditioning circuits, injection
from DG due to their improper control, saturation of magnetic components etc. The performance of
conventional PLLs, DSOGI-PLL and DSOGI-FLL is severely hampered in presence of the dc-offset. The
estimated frequency under such case is characterized by presence of low frequency component
superimposed on the average value. This aspect (frequency estimation in presence of the dc-offset) is not
fully explored. To target this issue, few methods have been reported [24-29]. However, they are complex
and/or suggested for single-phase system. Hence, in order to eliminate errors in frequency estimation
caused due to presence of the dc-offset and other grid abnormalities (e.g. unbalance, harmonics,
frequency variation, magnitude variation etc.), it is needed to investigate further into this area to provide a
better alternative of phase/frequency estimation under such non-ideal conditions.
3. Definition of the Problem
The injection of harmonics by the non-linear loads connected at the PCC and by other power
electronic converters in the grid may distort the source current and the voltage at the PCC in the modern
power system. The consumption of this current deteriorates the performance of the various electrical
equipments connected to the utility and reduces the life expectancy of them. The deteriorated quality of
voltages and/or currents further introduces the challenge in correct detecting the zero-crossing of the grid-
voltage and hence, its phase, frequency and magnitude estimation. Also, protective devices connected to
the utility may mal-operate. The major problem is faced by the power electronic converters, which
requires the accurate phase and frequency estimation of the grid voltages and currents for various
functions like active-reactive power control, harmonic mitigation, imbalance mitigation, improving
system stability etc., for which they are employed. This leads to the deviation in their operation from the
desired one and hence, lead to further deterioration of the power quality making the challenge of phase
and frequency estimation still complex. Different three phase time domain approaches based on PLL and
FLL have been studied so far to estimate positive sequence components as well fundamental frequency in
circumstances likes imbalance, frequency jump, phase jump, harmonics etc. in grid utility. However, this
estimation is affected if any dc-offset error is introduced to the sensed grid signal. This dc component
results due to inaccurate A/D conversion process, measurement errors, dc injection from distributed
generation systems, and so on. Hence, it is advisable to have a phase and frequency detection technique
that can accurately estimate the phase and frequency even when the voltage at the PCC is highly distorted
and bears non-idealities like harmonics, imbalance and dc-offset. Accordingly, the goal is set to provide
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a robust fundamental frequency/positive sequence extraction scheme to cope up the effect of the dc-offset
component.
4. Objective and Scope of work
The objective of the research area is summarized as under:
“To investigate the issues related to the modern power system which is characterized by the
presence of power electronic converters for applications like interfacing DGs, improving system
performance, and for meeting the need of modern domestic and industrial loads. As proper operation
of these converters require accurate phase (or frequency) and magnitude information of the grid
voltage and or currents for applications like synchronization, active-reactive power control, load
sharing, harmonic compensation etc., it is intended to devise a suitable PLL OR FLL scheme for
estimating the fundamental frequency/positive sequence components under non-ideal conditions (like
voltage unbalance, harmonics, dc-offset etc.), to enhance the performance of power electronics
converters and to utilize the scheme in designing control strategy for power electronic converters to
provide system support benefits like reactive power and harmonic current compensation.”
The scope of work includes:
1. To study and evaluate various fundamental frequency estimation/positive sequence extraction
techniques in terms of their capabilities to estimate the frequency when the grid voltage is
distorted (i.e. characterized by harmonics, imbalance, dc-offset)
2. To suggest and implement the fundamental phase angle estimation technique which can correctly
estimate the frequency under all such non-idealities.
3. To explore and prepare the performance comparison of these techniques using simulation in
MATLAB/Simulink and also to validate the same with experiments.
4. To evaluate the effect of these frequency estimation techniques on operation of power electronic
converters on one or more aspects like reactive power compensation, harmonic compensation,
synchronization, protection schemes of converters etc. through simulation and experimental
studies.
5. Original contribution by the thesis
The main contributions in the thesis are
1. Evaluation of various frequency estimation techniques in terms of their capability to estimate the
frequency when the grid/supply voltage is characterized by harmonics, imbalance and dc-offset.
With traditional frequency estimation techniques, the oscillatory response is observed in the
frequency estimation when the grid voltage has the dc-offset component.
2. Development, analysis and experimental verification of conventional and proposed method for
fundamental frequency/positive sequence components estimation under distorted grid conditions:
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The proposed modified DSOGI-FLL (MDSOGI-FLL) technique can eliminate the effect of
the dc-offset.
The performance is analyzed for different grid voltage conditions from the simulation as well
as experimental implementation.
3. Development, analysis and experimental verification of this proposed MDSOGI-FLL method for
estimating the reference compensating current for the SAPF
The performance is tested for different grid voltage conditions: ideal sinusoidal balanced grid
voltage, imbalance voltages with and without distortion, sinusoidal voltage with dc-offset,
imbalance voltages with dc-offset etc.
The simulation and experimental validation is carried out for grid tied SAPF.
It is highlighted that the SAPF based on modified DSOGI-FLL accurately tracks the
fundamental frequency as well positive sequence components under all conditions as
compared to traditional techniques. It gives satisfactory performance of the SAPF even when
grid voltage is characterized by the dc-offset.
6. Methodology of Research, Results / Comparisons
Various techniques that are available for the estimation of the frequency and magnitude of the grid
voltage/current are reviewed. The techniques can be classified as shown in the Fig. 1. Another way of
classification is based on whether they employ time or frequency domain approach. The time domain
techniques are very popular compared to the frequency domain techniques as they involve complexity in
implementation, gives better dynamic performance, and are robust in various grid abnormalities.
Fig. 1 Classification of synchronization scheme
Synchronization methods for converter sytems
Single-phase system Three-phase system
Closed-loop
Transport-
delay (T/4)
Inverse Park
transformation
Hilbert
transformation
EPLL
ANF
PSF
SSI
SOGI-PLL
SOGI-FLL
Kalman
Classical
single-phase
PLL
Enhanced PLL
(EPLL)
Vector-based
PLL
(based on
orthogonal
component
generation)
Modification
on
Classical
single-phase
PLL
ALOF-PLL
Fourier-
based PD
Symmetrical
component-
based PD
Adaptive
PLLClassical
SRF-PLL
Enhanced
PLL
(EPLL)
DFT based
Improvements/
Modifications
On
Classical SRF-PLL
Adding
filters
Extracting
symmetrical
components
Stationary
Reference
frame
Synchronous
rotating frame DDSRF-PLL
Neural-network
based
2nd order
LPF-based
Kalman
Adaline
LPF
MAF
Resonant
filter
DFT-based
controller
Notch filters
Closed-loop
Orthogonal
component-based
techniques
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6.1. Analyzing the performance of various frequency estimation techniques
Out of the various frequency estimation (or grid synchronization) techniques SRF-PLL and its
variants are widely employed [16]. Recently DSOGI-PLL due to its superiority over SRF-PLL has been
advocated by many researchers [17-18]. The comparison of fundamental frequency estimation algorithms
like SRF-PLL, DDSRF-PLL, DSOGI-PLL and DSOGI-FLL has been investigated using MATLAB
simulink modeling for three-phase system. The performance analysis of these techniques have been
investigated when the supply voltage experience imbalanced (single-phase sag) condition from healthy
condition at time t=0.1s. Also frequency jump in input signal (50 Hz to 45 Hz) occurs at t=0.25 s. The
tracking of the fundamental frequency 𝜔′ (rad/s) is accurately done by the DSOGI-FLL algorithm as
compared to other conventional PLL. Fig. 2 shows the relative performance of some of the frequency
estimation techniques. Apart from it, the performance of aforesaid algorithms is investigated when the
grid signal undergoes various abnormalities like phase jump, presence of harmonics components etc. The
performance of DSOGI-FLL for fundamental frequency estimation is superior for all type of grid
disturbances.
Fig. 2 Frequency estimation ω’ (rad/s) using different estimation algorithm in case supply voltage undergoes sag at time
t=0.15s and frequency step (50 Hz to 45 Hz) at 0.25s.
6.2 Proposed MDSOGI-FLL technique for frequency and magnitude estimation
This section presents the basic configuration of proposed MDSOGI-FLL. Fig. 3(a) shows structure of
basic conventional MDSOGI-FLL. The Clarke transformation is utilised to transform time-domain
signals from a natural three-phase coordinate system (abc) into a two-phase stationary reference frame
αβ0. The shaded block showing two MSOGI-QSG that represents modified dual second-order
generalized integrators is the key part of PLL or FLL structure. The details of MSOGI-QSG are shown in
Fig. 3(b). The y’’α and qy’’α signals forms a pair of quadrature signals where qy’’α lags y’’α by 90º. These
signals are used to extract positive sequence components through the Positive Sequence Calculator (PSC
shown in Fig. 3(a)) in the αβ stationary reference frame. The positive sequence components y’α and y’β
can be utilized to estimate the positive sequence (𝑦𝑎𝑏𝑐𝑠+ ) of the distorted grid input signal. A simple auto
tune block shown in Fig. 3(c) is used to adapt the center frequency 𝜔′ of the SOGI resonator to the input
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frequency. The frequency is estimated through the Frequency-Locked Loop (FLL) block in MDSOGI-
FLL and thus it discards the PLL block required in DSOGI-PLL. Hence, in the grid abnormalities like
sag, swell, variations, phase jump, harmonics etc., the MDSOGI-FLL performs extremely well, fast and
precisely as compared to conventional SRF-PLL and DSOGI-FLL based schemes. Fig. 3(b) shows the
DC-Loop’, which is added to the conventional SOGI to tackle the issue of dc-offset. For conventional
SOGI (i.e. in absence of the DC-loop), if the input voltage is characterized by the presence of the dc-
offset, the y’’β also contains dc-offset resulting into erroneous estimation of the frequency.
(a)
(b) (c) Fig. 3. Basic structure of MDSOGI-FLL: (a) abc to α
+β
+ computation (b) MSOGI-QSGs and (c) FLL-block.
It is worth noting from the above section that the conventional DSOGI-FLL fails to estimate the
frequency accurately when sensed grid signals are characterized by the dc-offset. The inclusion of third
integrator into the proposed MDSOGI-FLL structure shown in Fig.3 (a) results into large attenuation of
fundamental component (also higher order frequencies to a certain extent) allowing only the low order
frequencies to pass. Thus, it helps to estimate and eliminate the dc-offset accurately from input signals
vs/iL of Fig. 3(b).
The effectiveness of the proposed MDSOGI-FLL is demonstrated through the simulation results
obtained in MATLAB/Simulink. The parameter values used in the MDSOGI-FLL simulation model are
as follows: k1=1.28, kdc=0.26 and γ=40. The performance is evaluated when the supply voltage is having
abcyMSOGI
y
y
"y 'y
'y
PSC
'
"qy
"y
sT
MSOGI
2
1
2
1
2
1
2
1
"qy
'
Ls qiqv '/'
Ls iv /
1x
2x
dck
Ls iv '/'
DC Loop
1k'
x1
+
+
100C
.
2)(2)(
x2
num
den
k1
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imbalance along with the dc-offset. In Fig. 4, step change in amplitude of the grid signal is considered
only for phase ‘a’. At t=0.15s, the amplitude of phase ‘a’ voltage decreases from 1pu to 0.5pu. Also the
dc-offset of 0.1pu is introduced at t=0.15s. In addition, at t=0.25s frequency of grid signal suddenly
changes from 50Hz (314rad/s) to 45Hz (282.6rad/s). The ripple in the estimated frequency of DSOGI-
FLL is observed. The MDSOGI-FLL shows superior performance. As a result, the grid signal frequency
is quickly and accurately tracked. Apart from it, the positive sequence components y’α and y’β for
MDSOGI-FLL are free from offset, unlike that observed for DSOGI-FLL.
(a)
(b)
Fig. 4. Performance under unbalanced sag conditions: (a) Three-phase grid voltage signals. (b) Estimated frequency.
Table I shows the settling time for these frequency estimation techniques in response to a step change
in the frequency at t=0.25s. SRF-PLL and MDSOGI-PLL are relatively faster than other techniques. It
must be noted that except MDSOGI-FLL all other techniques show sustained oscillations in the estimated
frequency. Hence, the settling time for these techniques is determined as the time from the step change
till the estimated frequency waveform reaches a stage where sustained oscillations with a constant
average (dc) value is achieved. The proposed MDSOGI-FLL performs well on all the aspect even when
the dc-offset is present. Thus, it is not only fast but also accurate under all grid abnormalities.
TABLE I
TIME RESPONSE FOR DIFFERENT FREQUENCY ESTIMATION TECHNIQUES
PLL-type Estimated time
(ms)
Observed time
(ms)
SRF-PLL 40 50
DDSRF-PLL 40 70
DSOGI-PLL 40 45
DSOGI-FLL 40 60
MDSOGI-FLL 40 50
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The experimental results are included to validate the effectiveness of the proposed MDSOGI-FLL.
The different cases considered for simulation are verified experimentally using dSPACE DS1104 DSP
board as control system. The values of various parameters for which the MDSOGI-FLL is tuned are k1=
1.28. kdc=0.26 and γ=40, while those for DSOGI-FLL are k1 =1.41 and γ=100. The fundamental
frequency of the three-phase supply voltage and the sampling frequency are 50Hz and 10kHz,
respectively. The same parameters that are considered for simulation study carried out in
MATLAB/Simulink are adopted for experimental verification.
For the comparison of the proposed MDSOGI-FLL structure against the conventional DSOGI-FLL,
experimental results for one of the cases in which, voltage sag of 50% is introduced in just one of the
phases along-with the dc-offset in all the three phases, are shown in Fig. 6.. The three-phase unbalanced
voltage signals are shown in Fig. 5(a). Fig. 5(b) represents the comparison of the estimated frequency by
both these methods. Frequency obtained through DSOGI-FLL approach shows that the estimated
frequency is characterized by an oscillatory response, with a 100Hz frequency ripple. Frequency
estimated by MDSOGI-FLL not only is free from oscillations, but also has lower frequency dip
corresponding to sudden frequency decrease. Thus, the overshoot with the step response with MDSOGI-
FLL is less indicating a better transient response.
w’ (50 V/div)
Vabc
(5 V/div)
Frequency
Jump
25 ms/div
Single Phase
SagInitial Condition Regain
(a)
DSOGI-FLLMDSOGI-FLL
25 ms/div
(b)
Fig. 5. Experimental results with imbalance and dc-offset in supply voltage: (a) Three-phase grid voltage (b) Estimated
frequency with DSOGI-FLL and MDSOGI-FLL.
6.3 Harmonic mitigation with SAPF based on MDSOGI-FLL
The proposed MDSOGI-FLL is integrated with the instantaneous reactive power theory (p-q theory) to
design a control scheme for a SAPF, which can effectively operate even when grid-voltage is
characterized by abnormalities like, harmonics, imbalance, dc-offset etc. The details of the control
technique and the simulation and experimental set-up are explained next.
Fig.6 shows the system configuration of the MDSOGI-FLL based SAPF, which is connected at the
point of common coupling (PCC) to supply the harmonics generated by the non-linear load. As a non-
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linear load, a three phase uncontrolled rectifier feeding a resistive load (RL) is considered. The input
current, iLabc of the rectifier is characterized by the harmonics of the order 6n±1 (where n = 1, 2, 3...).
The SAPF injects compensation currents iCabc at the PCC through the coupling inductance Lf making the
supply current (isabc) free from the harmonics. In addition, the SAPF also supplies the reactive power
demand of the load to achieve a unity power factor operation of the grid (at the PCC). Semikron’s
Voltage Source Inverter (VSI) employing self-controlled Insulated Gate Bipolar Transistor (IGBTs)
switches S1 through S6, is used as the SAPF. The sensor card (LV-25-600) is used to sense dc bus
capacitor voltage vdc. Load current (iLabc) and the inverter output currents (iCabc) are sensed through
current transformers (CT) and processed through signal conditioning circuits before feeding to the
dSPACE MicroLabBox-1202.The supply voltage is stepped down through transformers and then fed to
dSPACE MicroLabBox-1202, which controls the VSI to act as the SAPF. The software implementation
Fig. 6 Circuit configuration of three-phase SAPF.
of reference current generation (RCG) and PWM hysteresis current control algorithm is implemented in
MATLAB/Simulink and fused in the processor of dSPACE MiroLabBox-1202 to finally generate the
switching signals, which are applied to the IGBTs of VSI through PWM isolator driver card (Edutech
Application Specific kit-30).
The control strategy employs the instantaneous power theory commonly known as p-q theory which
is being utilized to calculate the reference compensating current. The Clarke’s transformation transforms
these three-phase quantities to two-phase stationary reference frame voltages vsαβ0, and currents iLαβ0,
respectively. Apart from this, the reference current generation through the conventional DSOGI-FLL and
proposed MDSOGI-FLL is explained. However, it is very challenging task to calculate the reference
compensating current 𝑖𝐶,𝑎𝑏𝑐 ∗ when the utility is distorted by the various grid-load tie-up situation in
micro-grid, weak grid etc.
vdc
Cai
PW
M Iso
lato
r
Driv
er C
AR
D
Sig
nal S
en
sing
an
d
Pro
cessin
g C
ard
vsa
vsb
vsc
isa
isb
isc
iCa iCb iCc
iLa
iLb
iLcRL
iLa
iLb
iLc
vdc
VSI
Lf Lf Lf
C
PCC
iCa
iCb
iCc
S1--S6
E
dS
PA
CE
Mic
roL
abB
ox-1
202
G
C
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6.3.1. RCG based on MDSOGI-FLL
The calculation of reference current 𝑖𝐶,𝑎𝑏𝑐 ∗ is carried out through the p-q theory [5]. The three-phase
grid voltage vsabc (voltage at PCC) and three-phase load currents iLabc, are sensed and converted to
stationary reference frame (vsα , vsβ and iLα , iLβ in αβ reference frame) using Clarke’s transformation.
These two phase quantities are used to calculate the instantaneous active and reactive power as follows:
𝑝 = 𝑣𝑠∝ ∙ 𝑖𝐿𝛼 + 𝑣𝑠𝛽 ∙ 𝑖𝐿𝛽 = 𝑝 + 𝑝 (1)
𝑞 = 𝑣𝑠𝛽 ∙ 𝑖𝐿𝛼 − 𝑣𝑠𝛼 ∙ 𝑖𝐿𝛽 = 𝑞 + 𝑞 (2)
where, 𝑝 and 𝑝 represents the average and oscillating components of the instantaneous real power,
respectively. Similarly, 𝑞 and 𝑞 represents the average reactive power and oscillating components of the
instantaneous reactive power, respectively. The fundamental components of iLabc in the αβ reference
frame, 𝑖′𝐿𝛼 and 𝑖′𝐿𝛽 , depend only on the average active power and reactive power. Hence,
𝑖′𝐿𝛼 ,𝑝 and 𝑖′𝐿𝛽 ,𝑝 , the components of iLabc, that contribute only to average active power consumed by the
load are expressed by (3).
𝑖′𝐿𝛼 ,𝑝
𝑖′𝐿𝛽 ,𝑝 =
1
𝑣𝑠𝛼2 + 𝑣𝑠𝛽2
𝑣𝑠𝛼𝑣𝑠𝛽
𝑝 (3)
As the SAPF is intended to supply only the reactive power and harmonic currents, the reference
compensating current 𝑖𝐶,𝑎𝑏𝑐 ∗ is derived using (4).
𝑖𝐶𝑎𝑏𝑐 ∗ = 𝑖𝐿,𝑎𝑏𝑐 – [𝑖′𝐿,𝑎𝑏𝑐
] (4)
where 𝑖′𝐿,𝑎𝑏𝑐 is the obtained using αβ-abc transformation expressed by (5).
[𝑖′𝐿,𝑎𝑏𝑐
] =
𝑖′𝐿𝑎𝑖′𝐿𝑏𝑖′𝐿𝑐
=2
3
1 0
−1
2
3
2
−1
2− 3
2
𝑖′𝐿𝛼 ,𝑝
𝑖′𝐿𝛽 ,𝑝 (5)
To maintain the voltage vdc constant, it is required to compensate for the parasitic losses occurring in the
capacitor and the losses in the inverter. This can be achieved by using 𝑝 expressed by (6) in (3).
𝑝 = 𝑣𝑠𝛼 𝑖′𝐿𝛼 + 𝑣𝑠𝛽 𝑖′𝐿𝛽 + 𝑝𝑙𝑜𝑠𝑠 (6)
The term ploss represents the active power required to meet the losses of inverter and capacitor, to
regulate the voltage at dc-bus. It can be obtained through proportional-integral (PI) controller by
processing the difference of the reference and actual voltage at the dc-bus. The fundamental positive
sequence components vs (and iL) is obtained from MDSOGI-FLL structure mentioned in Fig. 3. Fig. 3 (a)
comprises of two modified SOGI, commonly known as dual SOGI (DSOGI) structure. It estimates
filtered in-phase and quadrature components y’α, and y’β of the measured quantity y. Thus, two such
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structures are used: one each for grid-voltages and load currents to obtain the in-quadrature components:
v’sα, and v’sβ for voltages and i’Lα and i’Lβ for currents. The αβ components derived from three-phase ‘abc’
signals using Clarke’s transformation are no longer sinusoidal under distorted supply conditions and
hence, may affect the reference current generation. Hence, the SOGI acts on these αβ components to filter
out the harmonics and to yield a set of in-quadrature sinusoidal signals (y” and qy”) at the fundamental
frequency. From these set of in-quadrature signals derived from the two SOGIs, which are even utilized
to estimate the frequency, the PSC y’α and y’β (v’sα, and v’sβ from grid voltages and i’Lα and i’Lβ from load
currents) are derived. The filtered in-quadrature positive sequence components, v’α, and v’β and i’Lα and
i’Lβ, are utilised in the instantaneous power theory, to compute the compensating current. Thus, in (6),
𝑣𝑠𝛼 and 𝑣𝑠𝛽 are replaced by v’sα, and v’sβ. i’Lα and i’Lβ are the positive sequence load current components
derived as shown in Fig. 3(b). Fig. 7 shows the reference current generation for the MDSOGI-FLL based
SAPF, which fundamental load current i’Labc is compared with the actual sensed load current iLabc to get
the iCabc*. The difference of this reference current and inverter output current iCabc is control via hysteresis
current control loop to obtain the six switching pulses.
Fig. 7 Reference current calculation block.
6.3.2 Simulation and experimental results analysis
RCG discussed in section 6.3.1 is employed for load harmonic compensation using the SAPF system
configuration of Fig. 6. The simulation results obtained using MATLAB/Simulink and the experimental
results with the prototype of Fig. 8 are included in this section. The system parameters are tabulated in
Table II. The performance evaluation is compared for both the conventional DSOGI-FLL and MDSOGI-
FLL reference current generation scheme to highlight the superior performance of the MDSSOGI-FLL
based SAPF.
TABLE II
SYSTEM PARAMETERS
Supply voltage (RMS) 110V (phase voltage), 50 Hz
Non linear load Three phase bridge rectifier with Resistive Load of RL = 90Ω
DC-link capacitor C = 1100µF
DC-link voltage 300 V
Coupling inductor Filter inductance Lf = 5 mH
Source impedance Rs = 0.02 Ω , Ls = 1µH
Inverter rating 25kVA
Eqa. (6)
'v
Li' Li'
pLi ,'
pLi ,'
αβ/ abc
Labci'
Labci
+
-
Cabci*
'v
-PI
Vdc*
Vdc
+ploss
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Fig. 8 Hardware setup for SAPF
Figs. 9 and 10 show the response of the SAPF with the DSOGI and MDSOGI based control
algorithms, respectively. Figs. 9(a) and 10(a) show supply voltage in which phase-a has a dc-offset of
10% of the fundamental phase-voltage (RMS). Phase-a further experiences a voltage sag of 20% at
t=0.3s. The SAPF is turned on at t=0.2s.
Fig. 9(b) and 10(b) show, that in-quadrature components vsα and vsβ for both the approaches are of
similar nature. The dc-offset is observed in vsα. In addition, after t=0.3s when the supply voltage is
unbalanced, the components vsα and vsβ, though sinusoidal are distinct in magnitudes. The dc-offset is
even present in v’sβ with the DSOGI structure as observed in Fig. 9(c). The reason behind the presence of
dc-offset in v’sβ is the inability of the DSOGI to attenuate the low frequency component from it. Unlike it,
Fig. 10(c) shows that both v’sα and v’sβ, obtained with the MDSOGI structure, are not only identical in
magnitude but also free from dc-offset. Similarly, DSOGI structure can yield sinusoidal i’Lα and i’Lβ [Fig.
9(e)] components from the non-sinusoidal components iLα and iLβ [Fig. 9(d)]. However, i’Lβ also shows the
dc-offset. The dc-offset also leads to the ripple (oscillation) of 100Hz in the estimated frequency [Fig.
9(f)]. This ultimately, affects the reference current generation, leading to offset in the grid current as well.
The THD analysis of the grid current (for phase-a) shown in Fig. 9(g) is displayed as Fig. 9(h). It shows
SEMIKRON VSI ModuledSPACE-MicroLabBox-1202
PWM Isolator Driver Card
Sensor Card
PCC
Bridge Rectifier
RL
Lf
PC
Linear Load
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the presence of dc-component. In addition, the 100Hz ripple in the estimated frequency results into 2nd
harmonic in the grid current leading to the THD of 5.82%.
Fig. 10(e) shows that just like v’sα and v’sβ the i’Lα and i’Lβ components obtained through the
MDSOGI structure is free from the dc-offset. The filtering effect of the ‘DC-loop’ shown in Fig. 3(b)
helps in removing the oscillations in the estimated frequency. Fig. 10 (f) shows the ripple-free estimated
frequency. As a result, it helps in accurately generating the reference compensating current, leading to a
sinusoidal source current which is free of dc-offset. Fig. 10(e) shows the source current while the
harmonic spectrum for the phase-a source current is shown in Fig. 10(g). The harmonic spectrum
confirms the absence of the dc component from the source current. Even the second harmonic is absent.
The THD of the current is noted as 3.57% with MDSOGI structure against the 5.82% observed with the
DSOGI structure.
Experimental results are included in form of Figs.11 through 13 to justify the superior performance of
MDSOGI-FLL based SAPF over that of DSOGI-FLL based SAPF. Fig. 11 shows the performance of
the DSOGI-FLL based SAPF when operating with unbalanced supply voltage (without any dc-offset).
Fig. 11(a) shows that phase-a voltage undergo sag of 20% of fundamental. It shows that, as soon as the
SAPF is activated, the grid current not only becomes sinusoidal but also remains in phase with the phase
voltage resulting into unity power factor operation. The components vsα and vsβ [Fig. 11(b)], obtained
through Clarke’s transformation on the supply voltages, are not identical. The current components iLα and
iLβ [Fig. 11(c)] are also not identical and deviate from sinusoidal conditions. However, the voltage
components v’sα and v’sβ [Fig. 11(b)], and the current components i’Lα and i’Lβ [Fig. 11(c)] are sinusoidal
and nearly equal in magnitude, demonstrating the filtering capability of the SOGI structure. As a result,
the frequency is correctly estimated and shows a constant value (ripple free) as shown in Fig. 11(d). The
harmonic spectrums for the uncompensated source current and the compensated source currents (i.e.
when SAPF is active) are shown in Figs. 11(e) and 11(f), respectively. Reduction of THD from 10.7% to
2.47% is observed with the incorporation of the SAPF.
Fig. 12(a) shows the 3-phase unbalanced supply voltage where the phase-a not only experiences sag
(20% of fundamental) but also has a dc-offset (10% of fundamental). Such offset may be present in a
weak grid. Even if it is not present in the utility voltage, it may enter into the computation due to the error
in sensing and processing the signals. The experimental results shown here consider that the offset is not
in the actual grid signal, but has resulted from measuring or signal processing errors. Thus, the
waveforms of Fig. 11(a) represents the sensed supply voltages. Unlike the earlier case, the dc-offset is
observed in vsα. As a result, the dc-offset is also observed in v’sβ [Fig. 11(b)]. Fig. 11(c) shows that the
offset is also reflected in the waveforms of iLα and i’Lβ. Hence, unlike the earlier case, the nature of the
estimated frequency ω’ is oscillatory in nature.
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Fig. 9 Simulation results for DSOGI-FLL based SAPF. Fig. 10 Simulation results for MDSOGI-FLL based SAPF.
vsa vscvsb
SAPF on Phase-a sag
dc-offset
v sab
c (V)
(a) vsa vscvsb
SAPF on Phase-a sag
dc-offset
v sab
c (V
)
(a)
vsα vsβ
v sαβ
(V)
(b) vsα vsβ
v sα
β (V
)
(b)
v’sαv’sβ
v’sα
β (V
)
(c) v’sα v’sβ
v’sα
β (V
)
(c)
iLα iLβ
i Lα
β (A
)
(d)
i Lα
β (A
)
iLα iLβ (d)
i’Lα
β (A
)
i’Lα i’Lβ (e)
i’L
αβ (A
)
i’Lα i’Lβ (e)
ω’ (rad/s)
Vdc (V)
(f)
ω’,
Vdc
ω’ (rad/s)
Vdc (V)
(f)
ω’,
Vdc
isa isb isc
i sa
bc
(A)
(g)
Time (s)
i sa
bc (
A)
isa isb isc
Time (s)
(g)
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Fig. 11(d) shows that the estimated frequency is having a ripple of 100Hz. The supply current is also
characterized by the dc-offset resulting into a higher THD of the source current. The harmonic spectrum
of source current is shown in Fig. 12(f), which displays THD of 5.94%. Thus, DSOGI based SAPF is
unable to negate the effect of the dc-offset resulting into the computation of an inaccurate compensating
current. This finally leads to a grid current with a dc-offset and higher THD.
Fig. 13 shows the performance with MDSOGI-FLL based SAPF. The similar test conditions, as
considered for results of Fig. 12, are maintained. The MDSOGI structure estimates the dc-offset
component present in the input signal through integral action of the DC-loop shown in Fig. 3. It is
illustrated through Fig. 13(b) that the waveform of v’sα and v’sβ are sinusoidal, free of dc-offset and
identical in magnitude. Even-though vsα is characterized by the presence of dc-offset, it is not observed in
either v’sα or v’sβ. The same is true for i’Lα and i’Lβ [Fig. 13(c)]. Unlike the earlier case [Fig. 12(d)], the
estimated grid-signal frequency shown in Fig. 13(d) is free from 100Hz ripple. Hence, MDSOGI-FLL
based SAPF accurately calculates the reference compensating current resulting into a source current with
lower THD [Fig. 13(f)]. Reduction of THD from 10.9% to 2.09% is observed when the MDSOGI-FLL
based SAPF is activated. Thus, the proposed MDSOGI based SAPF shows superior performance under
all types of grid voltage abnormalities.
vsa vsbvsc isa
SAPF off
vsβvsα
v’sα v’sβ
iLα iLβ i’Lα i’Lβ
(a) (b) (c)
w’
vdc
(d) (e) (f)
Fig. 11 Experimental results for DSOGI-FLL based SAPF with unbalanced supply voltage having no dc-offset error.
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vsavsb
vsc
isa
SAPF off
vsα vsβ
v’sα v’sβ
iLα iLβ i’Lα i’Lβ
(a) (b) (c)
w’
vdc
(d) (e) (f)
Fig.12 Experimental results for DSOGI-FLL based SAPF when the supply voltage is unbalanced and has dc-offset in phase-
a.
vsa vsbvsc
isa
v’sα v’sβ
vsα vsβ
iLα iLβi’Lα i’Lβ
(a) (b) (c)
w’
vdc
(d) (e) (f)
Fig.13 Experimental results for MDSOGI-FLL based SAPF with voltage sag and dc offset in phase-a.
iCa*
iCa
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7. Achievements with respect to objectives
The necessity of the phase angle estimation and synchronization using PLL techniques is required
for wide range of application power electronics converters i.e. synchronization, reactive power
compensation, distributed power generation, active power filtering, load sharing, activation of protection
schemes etc. Hence, it is essential that phase and supply frequency of the voltage/current should be
estimated accurately to achieve the desired objective for the various applications mentioned above.
The effects of the various non-idealities/abnormalities in the PCC voltage like harmonics, imbalance
and dc-offset on the various phase and frequency estimation schemes have been investigated.
Simulation results and experimental investigations have been included to highlight that most of the
techniques fail in presence of dc-offset in the sense voltage/current. [Publication 5]
The proposed MDSOGI-FLL included in this research article has a robust performance in estimating
the fundamental frequency and magnitude among all the PLL studied above in various grid
abnormalities, even in case when the PCC voltage has dc-offset. Publication [1-2]
Fig. 14 shows the comparison of different frequency estimation techniques when subjected to a step
change in the supply frequency. The supply voltage is considered to have the harmonics, unbalance
and the dc-offset. The comparison is carried out for ωn = 2π50 rad/s, ζ= 0.707 to have the settling
time of 40ms.
Fig. 14 Performance comparison of different frequency estimation methods.
The inability of the conventional schemes to estimate the phase and frequency correctly under the
non-ideal supply voltage conditions, affects the performance of the power electronic converters. To
evaluate the performance of these PLL schemes under non-ideal voltage conditions on converter’s
performance, simulation and experimental studies are performed for a 3-phase shunt active filter. It is
demonstrated that even the DSOGI-FLL, which is quite accurate in estimating the phase/frequency
and magnitude of a PCC voltage infected by harmonics, fails when the same PCC voltage is
characterized by the dc-offset. Publication [3]
The feature of the MDSOGI-FLL to work effectively even with the PCC voltage having harmonics,
imbalance and dc-offset is utilized to design a 3-phase active filter that gives better performance
under all such non-idealities. The performance is examined through simulation results as well as
experimentally with the real time implementation. Publications [4]
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8. Conclusion
This research article presents a MDSOGI-FLL algorithm to estimate the positive sequence components of
distorted grid signal having harmonics, imbalance and dc-offset. The proposed technique estimates the dc
component from the input signal and rejects its effect in fundamental frequency/positive sequence
components calculation. The estimation is relatively fast and accurate compared to other conventional phase
angle estimation techniques.
An active filter based on DSOGI-FLL is designed for harmonic components mitigation. Effect of any
offset error in measurement, data conversion processes (A/D or D/A) or in the grid voltage is nullified through
the proposed MDSOGI-FLL technique. Hence, positive sequence components are estimated correctly for
further calculation of reference current generation of SAPF. Experimental results justify the robustness of the
proposed technique in unbalanced grid voltage having the dc-offset component.
9. Copies of papers published and a list of all publications arising from the thesis
[1] K. R. Patil and Hiren H. Patel, “Modified dual second-order generalised integrator FLL for
synchronization of a distributed generator to a weak grid,” in Proc. 16th
Annu. Conf. IEEE-EEEIC,
June 2016.
[2] K. R. Patil and Hiren H. Patel, “Modified dual second-order generalized integrator FLL for frequency
estimation under various grid abnormalities,” in Transactions on Environment and Electrical
Engineering, vol. 1, no. 4, pp. 10-18, October-2016.
[3] K. R. Patil and Hiren H. Patel, “Performance of shunt active power filter with DSOGI-FLL under
distorted grid voltage,” in 2nd
Annu. Conf. IEEE- ICECCT, February 2017.
[4] K. R. Patil and Hiren H. Patel, “Shunt active power filter based on MDSOGI-FLL to address the issue
of dc-offset,” submitted to IEEE Tans. on Ind. Electronics.
[5] K. R. Patil and Hiren H. Patel, “Review of fundamental frequency estimation techniques for non-ideal
utility voltages ,” to be submitted to international coference/journal.
10. References
[1] J. Dixon, L. Moran, J. Rodriguez and R. Domke, “Reactive power compensation technologies: State-
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[2] R. N. Beres, X. Wang, M. Liserre, F. Blaabjerg and C. L. Bak, "A review of passive power filters for
three-phase grid-connected voltage-source converters," in IEEE Journal of Emerging and Selected
Topics in Power Electro., vol. 4, no. 1, pp. 54-69, Mar 2016.
[3] H. Akagi, “New trends in active filters for power conditioning,” in IEEE Trans. on Indu. Appl., vol.
32, no. 6, pp. 1312-1322, December 1996.
[4] H. Akagi, "Active Harmonic Filters," in Proceedings of the IEEE, vol. 93, no. 12, pp. 2128-2141,
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[5] H. Akagi, E. H. Watanabe, and M. Aredes, Instantaneous Power Theory and Applications to Power
Conditioning, M. E. El-Hawari, Ed. New York: Wiley, 2007.
[6] M. I. M. Montero, E. R. Cadaval and F. B. Gonzalez, "Comparison of control strategies for shunt
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[7] B. Singh and J. Solanki, "An implementation of an adaptive control algorithm for a three-phase shunt
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[9] P. Kanjiya, V. Khadkikar and H. H. Zeineldin, "A noniterative optimized algorithm for shunt active
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[10] P. Kanjiya, V. Khadkikar and H. H. Zeineldin, “Optimal control of shunt active power filter to meet
IEEE std. 519 current harmonic constraints under nonideal supply condition,” in IEEE Trans. on Ind.
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[11] D. Dinh, N. D. Tuyen, G. Fujita and T. Funabashi, “Adaptive notch filter solution under unbalanced
and/or distorted point of common coupling voltage for three-phase four-wire shunt active power filter
with sinusoidal utility current strategy,” in IET Generation, Transmission & Distribution, vol. 9, no.
13, pp. 1580-1596, January 2015.
[12] V. M. Moreno, A. P. Lopez and R. I. D. Garcias, "Reference current estimation under distorted line
voltage for control of shunt active power filters," in IEEE Trans. on Power Electron., vol. 19, no. 4,
pp. 988-994, July 2004.
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