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International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 4, No. 2, June 2014, pp. 173~191
ISSN: 2088-8694  173
Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS
Application of Backstepping to the Virtual Flux Direct Power
Control of Five-Level Three-Phase Shunt Active Power Filter
Bouzidi Mansour*,**
, Bouafia Saber**
, Bouzidi Ali***
, Benaissa Abdelkader**
, Barkat Said****
* Department of Electronics and Communications, Faculty of New Technologies of Information and Communication
University Kasdi Merbah, Ouargla, Algeria.
** Department of Electrical Engineering, Faculty of Engineering, University of Djilali Liabes, Sidi Bel Abbes, Algeria,
Intelligent Control Electronic Power System laboratory (I.C.E.P.S)
*** Department of Electrical Engineering, Faculty of Technology, University of Hadj Lakhdar Batna
**** Department of Electrical Engineering, Faculty of Engineering, M’sila University, M’sila, Algeria.
Article Info ABSTRACT
Article history:
Received Jan 11, 2014
Revised Mar 13, 2014
Accepted Mar 26, 2014
This paper proposes a virtual flux direct power control-space vector
modulation combined with backstepping control for three-phase five-level
neutral point clamped shunt active power filter. The main goal of the
proposed active filtering system is to eliminate the unwanted harmonics and
compensate fundamental reactive power drawn from the nonlinear loads. In
this study, the voltage-balancing control of four split dc capacitors of the
five-level active filter is achieved using five-level space vector modulation
with balancing strategy based on the effective use of the redundant switching
states of the inverter voltage vectors. The obtained results showed that, the
proposed multilevel shunt active power filter with backstepping control can
produce a sinusoidal supply current with low harmonic distortion and in
phase with the line voltage.
Keyword:
Five-level shunt active power
filter
Direct power control
Virtual flux concept
Backstepping control
Multilevel space vector
modulation
Copyright © 2014 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Bouzidi Mansour,
Department of Electronics and Communications,
Faculty of New Technologies of Information and Communication
University Kasdi Merbah, Ouargla, 30000, Algeria
Departement of Electrical Engineering,
Faculty of Engineering,
University of Djilali Liabes, Sidi Bel Abbes,
Sidi Bel Abbes 22000, Algeria
Email: bouzidi.m.28@gmail.com
1. INTRODUCTION
Nowadays the power electronic equipments are widely used in distribution networks which act as
nonlinear loads. Many power quality disturbances such as harmonics pollution, unbalanced load currents, and
reactive power problems are caused by the nonlinear loads; as a result poor power factor, weakening
efficiency, over heating of motors and transformers, malfunction of sensitive devices etc.
To overcome the aforementioned problems passive filters can be used to compensate some of them.
However, bulk passive components, series and parallel resonance and a fixed compensation characteristic are
the main drawbacks of passive filters [1]. Therefore, to give an effective solution for harmonics concerns
several active power filter (APF) topologies have been proposed. They aimed not only for current or voltage
compensation but also for voltage dips, flicker and imbalance [2].
Among various active filter configurations, the shunt active power filters (SAPF) have a number of
advantages [3]. Compared with the series and hybrid configurations, the SAPF do not need an additional
 ISSN: 2088-8694
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174
coupling transformer and require much less protection and switchgear. They operate as three-phase
controlled harmonic current sources and are not affected by harmonic distortions in supply voltages. In
general, the ratings of shunt active power filters are based on the magnitudes of compensating current and the
corresponding filter terminal voltage. For medium to high power applications the multilevel converters are
the most attractive technology. Indeed, multilevel converters have shown some significant advantages over
traditional two-level converters [4]-[7]. The main advantages of the multilevel converter are a smaller output
voltage step, lower harmonic components, a better electromagnetic compatibility and lower switching losses
[4]-[7]. In the recent time the use of multilevel inverters is prevailing in medium-voltage active power filters
without using a coupling transformer [8]-[11].
Various control strategies have been proposed to control the SAPF, such as hysteresis band current
control (HBCC) [12], voltage oriented control (VOC) [13]. Another interesting emerging control technique
called direct power control (DPC) has been investigated [13], [14]. DPC is based on the instantaneous active
and reactive power control loops. It is developed analogously with the well-known direct torque control
(DTC) used for adjustable speed drives. In DPC, there are no internal current loops or modulator block
because the converter switching states are selected via a switching table. Although DPC has many
advantages, some disadvantages of this control technique are high ripple content in the system current, high
ripple in the commanded active and reactive power, variable switching frequency, and requires a high
switching frequency [15].
The DPC can be forced to operate at a constant frequency by using space vector modulation (SVM)
to synthesize the space-vector voltage demanded by the switching table [15], [16]. Although classical DPC
uses the fix number of vectors present in this table, more vectors can be arbitrarily generated by using SVM.
In this way, the ripple in current can be reduced [15].
Recent developments have popularized the virtual flux (VF) concept, which assumes that both the
grid and converter’s line filter behave as an AC motor [17]. One of the main advantages of this approach is
that it is less sensitive to line-voltage variations than other approaches. The virtual flux direct power control
(VFDPC) is an adaptation of the DPC to a VF reference frame [17].
In this paper, a nonlinear control strategy based on the backstepping associated to VFDPC-SVM is
applied to three-phase five-level shunt power active filter in the aim to improve its performances.
In the present study, it is shown via simulation results that the proposed backstepping controller has
high performance both in the transient and in the steady state operations. The line currents are very close to
sinusoidal waveforms, a good control of the DC-bus voltage is obtained, and unity power factor operation is
achieved.
2. SHUNT APF CONFIGURATION
2.1. System Description
cv
av
bv
4C
1aS
2aS
1
2
3
4
4Cv
1aS
2aS
3aS
4aS
3aS
4aS
1bS
2bS
1bS
3bS
4bS
3bS
4bS
1cS
2cS
1cS
2cS
3cS
4cS
3cS
4cS
0
3Cv
2Cv
1Cv
4i
3i
2i
1i
0i
2bS
a
b
c
FaiFbiFci
Fau
Fbu
Fcu
3C
2C
1C
dcv
PCC
4Ci
3Ci
2Ci
1Ci
FR FL
FR FL
FR FL
sR
sR
sR LL
sci
sbi
saisL
sL
sL
LL
LRLai
Lbi
Lci LR
LR LL
sce
sbe
sae
lL
lR
Nonlinear
Load
Figure 1. Five-level shunt active power filter configuration
IJPEDS ISSN: 2088-8694 
Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
175
The structure in Figure 1, describes the proposed SAPF based on a three-phase five-level VSC. The
SAPF consists of three principal parts, the three-phase converter, four capacitors (C1, C2, C3, and C4) and the
smoothing inductances LF. The converter is used to charge and to discharge the capacitors to provide the
required compensating current.
The capacitors are used to store energy and the inductances LF are used to smooth and decrease the
ripples of the harmonic currents injected by SAPF [9].
The main task of the SAPF is to reduce harmonic currents and to ensure reactive power
compensation. Ideally, the SAPF needs to generate just enough reactive and harmonic current to compensate
the nonlinear load harmonic in the line. The resulting total current drawn from the AC main is sinusoidal.
2.2. Modeling of the PWM five-level inverter
The topology of the three-phase five-level NPC inverter is shown also in Figure 1. Here, xv and Fxi
, x = a, b, c, represent the point of common coupling (PCC) voltages and AC side currents, respectively. RF
is a line resistance that models the parasitic resistive effects of the inductor LF. The capacitances of input
capacitors are assume equal C1=C2=C3=C4=C. For a net dc-side voltage of vdc, each capacitor voltage is
ideally vCj = vdc/4, j = 1,..., 4 and each generated phase voltage uFx, x = a, b, c, has five levels with respect to
dc-side reference point 0. The switching states and the resultant phase voltages are listed in Table 1, where
state conditions 1 and 0 indicate ON and OFF switch status, respectively.
Table 1. Switching states of a five-level inverter
Switching
state
1S 2S 3S 4S 1S 2S 3S 4S Phase
voltage
4 1 1 1 1 0 0 0 0 dcv
3 0 1 1 1 1 0 0 0 3 / 4dcv
2 0 0 1 1 1 1 0 0 / 2dcv
1 0 0 0 1 1 1 1 0 / 4dcv
0 0 0 0 0 1 1 1 1 0
The switching functions of the five level inverter of Figure 1, are expressed as:
4 4 3 2 1
3 4 3 2 1
2 4 3 2 1
1 4 3 2 1
0 4 3 2 1
, ou
x x x x x
x x x x x
x x x x x
x x x x x
x x x x x
F S S S S
F S S S S
F S S S S x a b c
F S S S S
F S S S S


 


(1)
Referring all of the voltages to the lower DC-link voltage level (“0” reference), each output voltage consists
of contributions by a determinate number of consecutive capacitors:
4
0
0 0
, , ,i
j
x xj C
j i
u F v x a b c
 
 
  
 
  (2)
When balanced distribution of the DC-link voltage among the capacitors is assumed:
4
0
0
, , ,
4
dc
x xj
j
v
u jF x a b c

  (3)
The line to line voltage is given by:
0 0
0 0
0 0
ab a b
bc b c
ca c a
u u u
u u u
u u u
   
       
      
(4)
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176
The expressions of instantaneous inverter phase output voltages are given by:
1
3
Fa ab ca
Fb bc ab
Fc ca bc
u u u
u u u
u u u
   
       
      
(5)
2.3. Mathematical model of three-phase five levels SAPF
The mathematical equations which govern the behaviour of the ac-side of shunt active filter are:
1
( )
1
( )
1
( )
Fa
Fa a F Fa
F
Fb
Fb b F Fb
F
Fc
Fc c F Fc
F
di
u v R i
dt L
di
u v R i
dt L
di
u v R i
dt L
  
  
  
(6)
Where, , , ,Fiu i a b c represent voltages of the SAPF.
By transforming (6) in stationary frames, it follows that:
1
( )
1
( )
F
F F F
F
F
F F F
F
di
u v R i
dt L
di
u v R i
dt L

  

  
  
  
(7)
Where, v  and v  are the PCC voltages in the stationary α-β coordinates. Fi  and Fi  are α-β components
of AC currents of SAPF. Fu  and Fu  are α-β components of AC side voltages of SAPF.
The DC side of the filter can be expressed as:
1 2 3 4( )dc
C C C C
dv d
v v v v
dt dt
    (8)
Equation (8) can also be written as:
1 2 3 4
1
( )dc
C C C C
dv
i i i i
dt C
    (9)
Where iCj ( j =1,2,3,4) is the current through capacitor Cj.
The equation of DC side (9) can be related to the AC side by the following power-balance
relationship:
1 1 2 2 3 3 4 4C C C C C C C C a Fa b Fb c Fcv i v i v i v i v i v i v i      (10)
If we assume that the capacitor voltages are balanced, the equation (9) becomes:
1
( )dc
a Fa b Fb c Fc
eq dc
dv
v i v i v i
dt C v
   (11)
Where: / 4eqC C .
Equation (11) can be expressed as:
IJPEDS ISSN: 2088-8694 
Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
177
dc F
eq
dv p
dt C
 (12)
Where: pF is the instantaneous active power of SAPF.
F F Fp v i v i     (13)
3. NONLINEAR VIRTUAL FLUX BASED DIRECT POWER CONTROL
The backstepping VFDPC-SVM control strategy main scheme is presented in Figure 2. The
nonlinear load and SAPF currents are sensed using tow current sensors located in phases (a) and (b), and the
estimated PCC virtual flux components ,PCC PCC   are used for the powers estimation (pL, qL and pF, qF)
and backstepping power controller.
PCC
cv
bv
av
F refu F refu 
Lq
PCC
Fabci
abcS
Fabci
Fp FqFi 
Labci
3Cv
2Cv
1Cv
Li  Li 
Lp
Frefp
Frefp
Lp
1Cv
2Cv
C
C
C
C
Lci
Lbi
Lai
sR
sR
sR LL
FR
FR
FR FL
FL
FL
sci
sbi
saisL
sL
sL
LL
LR
LR
LR
Fai
Fci
Fbi
LL
sce
sbe
sae
lL
lR
abc

4Cv
3Cv
0Frefq 
abcS
abc

dcv
dcrefv
PCC
Figure 2. Backstepping VFDPC-SVM scheme of five-level SAPF
The active power pL is delivered to the high pass filter (HPF) to obtain the alternate values, which
finally are used as compensating component. The reactive power qL can be delivered to the HPF or
directly to the input of the backstepping power controller depending on compensation requirements
(compensation of higher harmonics or compensation of higher harmonics and reactive power at the
same time). The reference active power pFref (generated by the outer nonlinear DC voltage controller) and
reactive power reference qFref (set to zero for unity power factor) values are compared with estimated
instantaneous pF and qF values augmented by their corresponding alternate load powers pL and qL,
respectively. The errors are delivered to the backstepping power controller, which eliminates steady state
error. The output signals from backstepping power controller are used for switching signals generation by a
five-level space vector modulator [13].
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IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191
178
3.1. PCC virtual flux estimator
The principle of VF is based on assumption that the voltages imposed by the line power in
combination with the AC side inductors can be considered as quantities related to a virtual AC motor,
where RF and LF represent the stator resistance and leakage inductance of the virtual motor [17]. With
the definitions:
PCC vdt   (14)
In general RF can be neglected and the voltage v can be expressed as in stationary α- coordinates as follows:
F
F F
F
F F
di
v u L
dt
di
v u L
dt

 

 
 
 
(15)
The integrated of both sides of (15) gives:
PCC F F F
PCC F F F
u dt L i
u dt L i
  
  


 
 


(16)
The measured line currents ,F Fi i  and the estimated virtual flux components ,PCC PCC   are
used for SAPF power estimation.
3.2. Active and reactive powers estimator
Using the measured current and the estimated PCC virtual flux, the estimated active and reactive
powers can be described by the following formulas [17]:
a) Active filter powers are:
( )
( )
F PCC F PCC F
F PCC F PCC F
p i i
q i i
   
   
  
  
 
 
(17)
b) Nonlinear load powers are:
( )
( )
L PCC L PCC L
L PCC L PCC L
p i i
q i i
   
   
  
  
 
 
(18)
Where: ω is the angular frequency.
Both power estimation equations are simple to calculate and do not require the computation of the
current derivatives.
3.3. Active and reactive power model based on virtual flux
The backstepping power controller is based on instantaneous power time derivative behavior. From
Equation (17), the derivatives of active and reactive powers are given by:
F PCCPCC FF
F PCC F PCC
PCC FPCC FF
F PCC F PCC
di dd didp
i i
dt dt dt dt dt
d did didq
i i
dt dt dt dt dt
  
   
  
   

  

  
 
    
 
 
    
 
(19)
For three-phase balanced system, the following relations can be written:
IJPEDS ISSN: 2088-8694 
Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
179
,
,
PCC
PCC PCC
PCC
PCC PCC
v d
dt
dv
dt
 
 

 

 


 

  
  
(20)
Replacing (7), (20) into (19), power derivatives can be expressed as:
 
 
 
 
PRCF
F F F PRC F
F
PRC
F F PRC F
F
PRCF
F F F PRC F
F
PRC
F F PRC F
F
dp
q R i u
dt L
R i u
L
dq
p R i u
dt L
R i u
L

  

  

  

  

 



 


     
   
    
   
(21)
3.4. Backstepping controllers design
Backstepping is a systematic and recursive design methodology for nonlinear feedback control. This
approach has emerged as powerful tools for stabilizing nonlinear systems both for tracking and regulation
purposes [18]. The backstepping algorithm takes advantage of the idea that certain variables can be used as
virtual controls to make the original high order system simple, thus the final control outputs can be derived
step by step through suitable Lyapunov functions ensuring global stability. This control method has been
successfully applied on a growing collection of plant. However, few papers are devoted to the backstepping
control of power electronics converters [19]-[20]. In the following, the backstepping design procedure is
applied to five-level shunt active power filter. As chosen in Figure 2, the control strategy is based on a
cascade structure, namely, the output of outer voltage loop is used as reference signal in the inner power
loop.
The approach adopted herein designs by breaking down a complex nonlinear system into smaller
sub-systems, then designing control Lyapunov functions and virtual controls for these sub-systems. In order
to design the control algorithm for active power filter with the aid of backstepping method, nonlinear
differential Equation (12) and (21) must be portioned in three SISO subsystems at the following form:
( ); 1,2,3
k kk f k g k k
k k k
L h L h u
y h k


 
 

(22)
Where k , ku and ky represent state, control input and output of kth
system, respectively. kf and kg are
smooth fields, and kh is a smooth scalar function. The term kf kL h stands for the Lie derivative of kh with
respect to kf , similarly kg kL h .
By identifying the first subsystem, based on equation (12), with (22), it can be yield:
1
1
1 1 1 1 1
1
, , y , 0
1
dc F dc f
g
eq dc
v u p h v L h
L h
C v
     

(23)
The second and the third subsystems are built based on the active and reactive derivative (21).
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180
The identification of (21) with (22) leads to:
 
   
 
 
2
2
3
2 2
2 2 2
2
3 3
3 3 3
3 3
,
, 1
,
, 1
F F PCC F PCC F
F
F g
f F PCC F F PCC PCC F F PCC
F
F F PCC F PCC F
F
F g
f F PCC F F PCC PCC F F
F
p u u u u
L
y h p L h
L h q R i R i
L
q u u u u
L
y h q L h
L h p R i R i
L
    
     
    
    

  

    

  

    
    
  
         
   
  
       PCC
 
 
(24)
In following sections the backstepping method will be used for developing the dc voltage and power
controllers.
3.4.1. DC Voltage Controller Synthesis
In order to ensure that the SAPF operates effectively it is important to maintain the dc capacitor
voltage at a constant desired value. The backstepping dc voltage controller sets the active power of the
inverter to regulate the dc voltage based on its reference value covering the inverter losses.
The purpose of this control is to achieve the dc voltage reference, so the first tracking error is
defined as:
1 1 1dz y y  (25)
Where:
1d dcrefy v
Differentiating (25) with respect to time, it is obtained that:
1 11 1 1 1f g Fref dz L h L h p y    (26)
The candidate function of Lyapunov is chosen as:
2
1 1
1
2
V z (27)
The derivative of the Lyapunov function is expressed as:
1 11 1 1 1 1 1 1( )f g Fref dV z z z L h L h p y     (28)
To guarantee the Lyapunov stability, the control law is chosen as:
1
1
1 1 1 1
1
f d
Fref
g
k z L h y
p
L h
  


(29)
Where, k1 is a positive constant.
3.4.2. Power Controller Synthesis
Using the backstepping approach, one can synthesize the control law forcing the active and reactive
powers to follow the desired powers.
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181
For the first step the following tracking-errors are considered:
2 2 2
3 3 3
d
d
z y y
z y y
 
 
(30)
Where:
2 _
3 _
d Fref total
d Fref total
y p
y q


Where:
_
_
Fref total Fref L
Fref total Fref
p p p
q q
 


(31)
The resulting error dynamics equation can be expressed as:
2 2
3 3
2 2 2 2
3 3 3 3
f g F ref d
f g F ref d
z L h L h u y
z L h L h u y


  
  


(32)
The chosen Lyapunov functions are given by the following expressions:
2
2 2
2
3 3
1
2
1
2
V z
V z


(33)
The time derivatives of Lyapunov functions 2 3andV V are given by:
2 2
3 3
2 2 2 2 2 2 2
3 3 3 3 3 3 3
( )
( )
f g F ref d
f g F ref d
V z z z L h L h u y
V z z z L h L h u y


   
   
 
 
(34)
In order to make negative the derivatives of Lyapunov functions, the intermediate control laws
F refu  and F refu  are proposed in the following equation:
2
2
3
3
2 2 2 2
2
3 3 3 3
3
f d
F ref
g
f d
F ref
g
k z L h y
u
L h
k z L h y
u
L h


  

  



(35)
Where, k2 and k3 are positive constants.
The relation between the intermediate and final control laws is given by:
F ref F ref
F ref F ref
u u
D
u u
 
 
   
   
   
(36)
Where:
PRC PRC
PRC PRCF
D
L
 
 
 
 
 
  
 
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182
The D matrix determinant is different to zero, so the final control laws are given as:
1F ref F ref
F ref F ref
u u
D
u u
 
 
   
   
   
(37)
3.5. Space Vector Modulation with DC-Capacitor Voltages Balancing Strategy
In the five-level NPC topology, the voltages of the four series-connected dc-link capacitors must be
confined to vdc/4 to take advantage of the inverter. The dc-voltage backstepping control regulates only the
total dc voltage. For this reason, the dc-capacitor voltages are kept equals using five-level SVPWM that takes
advantages of redundant switching states to counteract the dc voltages drift phenomenon [21].
The five-level SVPWM technique can approximate the reference voltage vector, computed by
backstepping power controller, using the nearest three vectors. They are selected to minimize the energy of
the dc-capacitor voltages [21].
Figure 3 represents the space vector states for the five-level inverter there are 125 switching-state
vectors. Applying Clark’s transformation to all combinations of output voltages associated with the 125
switching-state vectors results in 60 nonzero voltage space vectors.
Projection of the vectors on αβ coordinates forms a four-layer hexagon centered at the origin of the
αβ plane (Figure 3), and zero-voltage vectors are located at the origin of the plane.
1st
Sector
1
1
f g
Frefu
m
o
n
lj k
1
s
u
a b c d e
h i
1
1Frefu
1
2Frefu
2
s
u
400
440
410
420
430
411
300
421
310
431
320
441
330
422
311
200
432
321
210
442
331
220
433
322
211
100
443
332
221
110
000
111
222
333
444
343
232
121
010
344
233
122
011
434
323
212
101
334
223
112
001
342242
231
120
131
020
243
132
021
244
133
022
423
312
201
234
123
012
424
313
202
324
213
102
224
113
002
341241141
030 130 230
142
031
143
032
144
033
134
023
412
301
413
302
414
303
124
013
314
203
214
103
114
003
041
340240140040
042
043
044
034
024
401
402
403
404304204104004
014
2nd
Sector
3rd
Sector
4th
Sector
5th
Sector
6th
Sector

F refu 
F refu 

1
2
1
3
1
4
1
5
1
6
1
7
1
8
1
10
1
9
1
11
1
12
1
13
1
14
1
15
1
16
Figure 3. Space voltage vectors for a five-level inverter
3.5.1. Determination of the Space Vector Location
The space vector location is determined in two steps. The first step determines the sector number of
where the vector lies. The second step determines the triangle in which the vector lies [22].
Step 1: Sector number computation.
The reference voltage vector magnitude and its angle are determined from:
2 2
Fref F ref F refu u u   and 1
tan 2
F ref
F ref
u
u


 
 
   
 
(38)
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Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
183
Where, the tan 2-1
function returns the four-quadrant inverse tangent. Once the value of  is calculated, the
sector numbers are given by [22]:
 ceil 1,2,3,4,5,6
/ 3
S


 
  
 
(39)
Where ceil is the C-function that adjusts any real number to the nearest, but higher, integer.
Step 2: Triangle identification.
Reference vector Frefu is projected on the axes of 60° coordinate system [21]. In each sector S, the
normalized projected components are 1
s
Frefu and 2
s
Frefu given by (40). Fig. 3 shows the projection of Frefu in
the first sector.
1
2
cos( ( 1) )) sin( ( 1) )
3 33
2
3 2
2
sin( ( 1) )
33
2
3 2
Fref
Fref
S
Fref
dc
Fref
S
Fref
dc
u
u S S
u
v
u S
u
v
 
 


    

 

(40)
In order to identify the triangle where the required reference is located, the following integers are
used:
 
 
1 1
2 2
int
int
S S
Fref
S S
Fref
l u
l u


(41)
Where the int() function returns the nearest integer that is less than or equal to its argument. The triangle
number is obtained according to the value of 1
S
l and 2
S
l , as shown in Table 2:
Table 2. Triangle identification in each sector S
1
S
l 2
S
l  ( 1,...,16 )S
i i 
0 0
16 1 2Si ( 1)S S S
ref refu u  
14 1 2Si ( 1)S S S
ref refu u  
1 0
13 1 2Si ( 2)S S S
ref refu u  
9 1 2Si ( 2)S S S
ref refu u  
2 0
8 1 2Si ( 3)S S S
ref refu u  
2 1 2Si ( 3)S S S
ref refu u  
3 0
1
S

0 1
15 1 2Si ( 2)S S S
ref refu u  
11 1 2Si ( 2)S S S
ref refu u  
1 1
10 1 2Si ( 3)S S S
ref refu u  
4 1 2Si ( 3)S S S
ref refu u  
2 1
3
S

0 2
12 1 2Si ( 3)S S S
ref refu u  
6 1 2Si ( 3)S S S
ref refu u  
1 2
5
S

0 3
7
S

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184
3.5.2. Duration Time Calculation
On-duration time intervals of the switching voltage vectors adjacent to the reference voltage vector
Frefu of a five-level NPC are calculated as follows:
s s s s s s
i i i i i i
s s s
i i i
x x y y z z Fref s
x y z s
u t u t u t u T
t t t T
     
  
  
  
(42)
Where Ts is the switching period,
s
i
xu 
,
s
i
yu 
and
s
i
zu 
are the three switching vectors adjacent to the reference
voltage vector located in the triangle ( 1,...,16)s
i i  formed by the vertices (x,y,z) and
s
i
xt 
,
s
i
yt 
and
s
i
zt 
are
the calculated on-duration time intervals of the switching vectors, respectively.
Expression (42) can by decomposed in the 60° coordinates system as follows:
1 1 1 1
2 2 2 2
s s s s s s
i i i i i i
s s s s s s
i i i i i i
s s s
i i i
x x y y z z Fref s
x x y y z z Fref s
x y z s
u t u t u t u T
u t u t u t u T
t t t T
     
     
  
  
  
  
(43)
The coordinates of all vertices of Sth
sector are given in Table 3.
Table 3. Vertices coordinate in Sth
sector
vertices coordinates
A
1 2( , ) (0,0)
S S
i i
A Au u 

B
1 2( , ) (1,0)
S S
i i
B Bu u 

C
1 2( , ) (2,0)
S S
i i
C Cu u 

D
1 2( , ) (3,0)
S S
i i
D Du u 

E
1 2( , ) (4,0)
S S
i i
E Eu u 

F
1 2( , ) (0,1)
S S
i i
F Fu u 

G
1 2( , ) (1,1)
S S
i i
G Gu u 

H
1 2( , ) (2,1)
S S
i i
H Hu u 

I
1 2( , ) (3,1)
S S
i i
I Iu u 

J
1 2( , ) (0,2)
S S
i i
J Ju u 

K
1 2( , ) (1,2)
S S
i i
K Ku u 

L
1 2( , ) (2,2)
S S
i i
L Lu u 

M
1 2( , ) (0,3)
S S
i i
M Mu u 

N
1 2( , ) (1,3)
S S
i i
N Nu u 

O
1 2( , ) (0,4)
S S
i i
O Ou u 

Substituting the coordinates of ux, uy and uz from Table 3 in (43), in each triangle, the on-duration
time intervals are summarized in Table 4. These duration times are valid in all sectors.
The significant outcome of the proposed algorithm is its inherent simplicity. Unlike the conventional
SVM algorithm that requires solution of several sets of trigonometric equations for calculation of on-duration
time intervals. Therefore, the proposed SVM algorithm is much simpler and easier for digital implementation
since it reduces the hardware and software complexity and decreases the required computational time.
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185
Table 4. Duration time in each triangle of the Sth
sector
Duration time intervals
Triangle
S
i
xt S
i
yt S
i
zt
1 ( , , ) ( , , )S
x y z D E I 
S S
i i
s y zT t t 
   1 3S
ref su T 2
S
ref su T
2 ( , , ) ( , , )S
x y z I H D 
S S
i i
s y zT t t 
   13 S
ref su T  21 S
ref su T
3 ( , , ) ( , , )S
x y z H I L 
S S
i i
s y zT t t 
   1 2S
ref su T  2 1S
ref su T
4 ( , , ) ( , , )S
x y z L K H 
S S
i i
s y zT t t 
   12 S
ref su T  22 S
ref su T
5 ( , , ) ( , , )S
x y z K L N 
S S
i i
s y zT t t 
   1 1S
ref su T  2 2S
ref su T
6 ( , , ) ( , , )S
x y z N M K 
S S
i i
s y zT t t 
   11 S
ref su T  23 S
ref su T
7 ( , , ) ( , , )S
x y z M N O 
S S
i i
s y zT t t 
  1
S
ref su T  2 3S
ref su T
8 ( , , ) ( , , )S
x y z C D H 
S S
i i
s y zT t t 
   1 2S
ref su T 2
S
ref su T
9 ( , , ) ( , , )S
x y z H G C 
S S
i i
s y zT t t 
   12 S
ref su T  21 S
ref su T
10 ( , , ) ( , , )S
x y z G H K 
S S
i i
s y zT t t 
   1 1S
ref su T  2 1S
ref su T
11( , , ) ( , , )S
x y z K J G 
S S
i i
s y zT t t 
   11 S
ref su T  22 S
ref su T
12 ( , , ) ( , , )S
x y z J K M 
S S
i i
s y zT t t 
  1
S
ref su T  2 2S
ref su T
13( , , ) ( , , )S
x y z B C J 
S S
i i
s y zT t t 
   1 1S
ref su T 2
S
ref su T
14 ( , , ) ( , , )S
x y z G F B 
S S
i i
s y zT t t 
   11 S
ref su T  21 S
ref su T
15 ( , , ) ( , , )S
x y z F G J 
S S
i i
s y zT t t 
  1
S
ref su T  2 1S
ref su T
16 ( , , ) ( , , )S
x y z A B F 
S S
i i
s y zT t t 
  1
S
ref su T 2
S
ref su T
3.5.3. DC-capacitor Voltages Balancing Based on Minimum Energy Property
In a five-level NPC inverter, the total energy E of dc-link capacitors is:
4
2
1
1
2 jj C
j
E C v

  (44)
When all capacitor voltages are balanced, the total energy E reaches its minimum of
2
min 8dcrefE Cv , with dcrefv is the desired value of dc voltage. This condition is called the minimum energy
property which can be used as the basic principle for dc-capacitor voltages balancing and control [21]. The
adopted control method should minimize a quadratic cost function J associated with voltage deviation of the
dc-capacitors. The cost function is defined as follows:
24
1
1
2 4j
dc
C
j
v
J C v

 
  
 
 (45)
The mathematical condition to minimize J is:
4
1
0j jC C
j
v i

  (46)
Where:
/ 2, 1,2,3,4Cj Cj dcv v v j   
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186
The capacitor currents are affected by the dc-side intermediate branch currents, i1, i2 and i3. Thus, it
is advantageous to express (46) in terms of i1, i2 and i3. The dc-capacitor currents are expressed as:
3 3
1
1
, 1,2,3,4.
4j
S S
C x x
x x j
i xi i j
 
    (47)
By substituting (47) in (46), the condition to achieve voltage balancing is deduced as:
4 3 3
1 1
1
0
4j
S S
C x x
j x x j
v xi i
  
 
   
 
   (48)
When the DC link voltages vCj are closed to their reference vdc /4, the following condition is verified:
4
1
0jC
j
v

  (49)
Using (49), the Equation (48) can be written as:
3 3
1
0j
S
C x
j x j
v i
 
 
  
 
  (50)
Applying the averaging operator, over one sampling period, to (50) results in:
( 1) 3 3
1
1
0
s
j
s
k T
S
C x
j x js kT
v i dt
T

 
  
   
   
  (51)
Assuming that sampling period Ts, as compared to the time interval associate with the dynamics of
capacitor voltages, is adequately small, the capacitor voltages can be assumed to remain constant over one
sampling period [21] and, consequently, (51) is simplified to:
3 3
1
( ) ( ) 0j
S
C x
j x j
v k i k
 
 
  
 
  (52)
Where, ( )Cjv k is the voltage drift at sampling period k, and , 1,2,3ji j  is the averaged value of the ji .
The current ji should be computed for different combinations of adjacent redundant switching
states over a sampling period and the best combination which maximizes (52) is selected.
4. SIMULATION RESULTS
The proposed backstepping controller for three-phase five-level SAPF has been simulated and
compared with conventional PI controller. The parameters used are shown in Table 5.
Table 5. Basic parameters of the system under study
RMS value of phase voltage 5.5 kV
DC-link capacitor C 5 mF
Source impedance Rs, Ls 0.1 mΩ, 0.1 mH
Filter impedance RF, LF 0.1 mΩ, 1 mH
Switching frequency fs 4 kHz
Fundamental frequency f 50 Hz
DC-link voltage reference vdc ref 20 kV
Diode rectifier load Rl , Ll 200 Ω, 1mH
Input diode rectifier impedance RL, LL 100 mΩ, 1 mH
Sampling frequency 1 MHz
k1, k2, k3 constants 70, 2.105
, 2.105
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Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
187
The goal of the simulation is to examine the capability of the controller to fulfill the following four
different aspects.
a) Harmonic current compensation
b) Dynamic response performance
c) Parameters variation
d) Distorted grid phase voltage
4.1. Harmonic Current Compensation
The AC supply current of phase (a) and its harmonic spectrums before and after compensation are
illustrated in Figure 4, 5 and 6. It results that the SAPF decreases the total harmonic distortion in the supply
currents from 29.68% to 2.96% with PI control and to 1.47 % with backstepping control. So, the distortion in
supply current with backstepping control is less than in case of PI control method.
Figure 4. (a) Supply current before harmonics compensation, (b) Its harmonic spectrum
Figure 5. (a) Supply current after harmonics compensation using backstepping controller, (b) Its harmonic
spectrum
Figure 6. (a) Supply current after harmonics compensation using PI controller, (b) Its harmonic spectrum
4.2. Dynamic Response Performance
In this section, the performances of the backstepping and PI controllers are analyzed under
100% step charge in the resistance load at t = 0.5s.
0.2 0.205 0.21 0.215 0.22
-150
-100
-50
0
50
100
150
Time (s)
isa
(A)
(a)
0.2 0.205 0.21 0.215 0.22
-200
-100
0
100
200
Time (s)
i
sa
(A)
(a)
0.2 0.205 0.21 0.215 0.22
-200
-100
0
100
200
Time (s)
i
sa
(A)
(a)
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188
Figure 7. Simulation results of the proposed VFDPC-SVM using backstepping controller. (a) Source current.
(b) Reduced source voltage and source current of a-phase (c) PCC active and reactive powers. (d) DC-link
voltage vdc. (e) DC capacitors voltages
The dynamic behavior under a step change of the load is presented in Figure 7 and 8 for
backstepping and PI controllers respectively. The active power was changed stepwise from 1.7 to 3.4 MW.
For clarity, a phase-a current is shown for illustration and the corresponding phase voltage is scaled down by
a factor of 1/20. It can be observed that the unity power factor operation is successfully achieved, even in this
transient state. As a result, the DC-bus voltage decreases, since the DC capacitors discharge. In a short time,
the backstepping controller starts to respond due to the voltage error signal, which is the difference between
the DC-bus reference voltage and the DC bus actual voltage. The output reference power of the controller
will increase slowly to attain the required active power.
When, the instantaneous value of the active power drawn from the grid is equivalent to the active
power consumed by the load, the DC-bus voltage stops decreasing and the inverter stops supplying the active
power. Afterwards, the DC-bus voltage returns to the value according to the DC-bus reference voltage
(without overshoot with backstepping control). When the DC-bus voltage is at its reference value, the new
steady state has been achieved with new grid current amplitude.
From Figure 7(e), it is important to note that the application of the proposed redundant vectors based
five-level SVM control maintains these voltages constant around the reference of 5kV.
0 0.2 0.4 0.6 0.8 1
-400
-200
0
200
400
Time (s)
i
sa
(A)
(a)
0.46 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54
-400
-200
0
200
400
Time (s)
e
a
(V)andi
sa
(A)
(b)
0 0.2 0.4 0.6 0.8 1
-1
0
1
2
3
4
5
x 10
6
Time (s)
p
PCC
(W)andq
PCC
(Var)
(c)
0 0.2 0.4 0.6 0.8 1
1.94
1.96
1.98
2
x 10
4
Time (s)
v
dc
anditsreference(V)
(d)
0 0.2 0.4 0.6 0.8 1
4850
4900
4950
5000
5050
5100
Times (s)
Capacitorsvoltages(V)
(e)
v
c4
v
c3
v
c2
v
c1
IJPEDS ISSN: 2088-8694 
Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
189
Figure 8. Simulation results of conventional VFDPC-SVM using PI controller. (a) Source current. (b)
Reduced source voltage and source current of a-phase (c) PCC active and reactive powers. (d) DC-link
voltage vdc. (e) DC capacitors voltages
3.3. Parameters Variation
The values of the inverter-side inductors LF may vary according to the operation point and aging. A
small variation in this parameter may cause erroneous virtual-flux estimation, and consequently, an incorrect
amount of active and reactive powers is generated by the inverter. To show the influence of these variations
in system accuracy, simulations with different inductor values are analyzed, Figure 9(a).
The switching frequency is also a biasing factor on the harmonic quality of the line current as well
as the size of SAPF inductances [23-24]. It is important to show its influence on the line current THD, Figure
9(b)
Figure 9. Simulation results of robustness examination. (a) THD of line current versus value of SAPF
inductor (b) THD of line current versus value of switching frequency.
0 0.2 0.4 0.6 0.8 1
-400
-200
0
200
400
Time (s)
i
sa
(A)
(a)
0.46 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54
-400
-200
0
200
400
Time (s)
e
a
(V)andi
sa
(A)
(b)
0 0.2 0.4 0.6 0.8 1
1.96
1.98
2
2.02
x 10
4
Time (s)
v
dc
anditsreference(V)
(d)
0 0.2 0.4 0.6 0.8 1
-1
0
1
2
3
4
5
x 10
6
Time (s)
p
PCC
(W)andq
PCC
(Var)
(c)
0 0.2 0.4 0.6 0.8 1
4900
4950
5000
5050
Time (s)
Capacitorsvoltages(V)
(e)
v
c4
v
c3
v
c2
v
c1
1 2 3 4 5 6 7
1
2
3
4
5
6
7
L
F
(mH)
THD(%)
(a)
Backstepping
PI
1 2 3 4 5 6 7 8 9 10
1
2
3
4
5
6
7
Switching frequency (kHz)
THD(%)
(b)
Backstepping controller
PI controller
 ISSN: 2088-8694
IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191
190
Figure 9(a) shows that the THD increases with the increase of the coupling inductance LF. The
proposed VFDPC-SVM using backstepping controller gives the best results for all values of LF. However, for
conventional VFDPC-SVM, the increase of LF leads immediately to the increase in current THD.
From the Figure 9(b) one notices well that the THD decreases remarkably with increase of the
switching frequency. It can be concluded that the VFDPC-SVM based on backstepping controller can be
operated with reduced switching frequency (1 kHz).
3.4. Distorted Grid Phase Voltage
In an ideal situation, the grid usually consists of a balanced three-phase power system with
sinusoidal line voltage-waves. However, the line voltage is frequently distorted and the systems which are
connected to the grid should be able to tolerate this situation. One of the main disturbances is the presence of
line voltage harmonics of order 5, 7 and 11. Figure 10 shows the waveforms in which a fifth harmonic
voltage component of 10% is intentionally superimposed on the fundamental grid voltage.
Figure 10. Simulation results of proposed backstepping VFDPC-SVM control with distorted grid phase
voltage. (a) Three-phase grid voltages. (b) PCC virtual flux. (c) Reduce source voltage and source current of
a-phase. (d) Harmonic spectrum of line current.
It can be observed that the grid current is nearly sinusoidal shape (THD = 3.21%) and unity power
factor operation is successfully achieved even in existence of the distorted grid voltages as shown in Figure
10. This result is due to fact that voltage was replaced by virtual flux (the integrator behaves like a low-pass
filter).
5. CONCLUSION
This paper has investigated a virtual flux direct power control based on backstepping approach for
three-phase shunt active power filter using a five-level inverter. The proposed control scheme is intended to
achieve harmonics elimination, reactive power compensation, and dc voltage regulation. Simulation results
show that the backstepping-based control strategy significantly reduces the current distortion to values
allowed by international standards, and regulates the power factor observed in the common coupling point
between the nonlinear load and the power distribution system as well as exhibits excellent transient response
during large load variations. When compared to the conventional control, the backstepping control offers
substantial improvements on harmonic content of supply current, and robustness to the filter parameters
variations. These results confirm that the backstepping control strategy provides higher performance than the
0 0.005 0.01 0.015 0.02
-1
-0.5
0
0.5
1
x 10
4
Time (s)
Threephasegridevoltages(v)
(a)
0 0.005 0.01 0.015 0.02
-30
-20
-10
0
10
20
30
Time (s)
VirtualfluxPCCestimation(Wb)
(b)
0.285 0.29 0.295 0.3 0.305 0.31 0.315
-500
0
500
Time (s)
v
a
(V)andi
sa
(A)
(c)
IJPEDS ISSN: 2088-8694 
Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour)
191
traditional control. Thus, the proposed method can be useful to different applications such as motor drives,
wind generators and power supply networks interconnection.
REFERENCES
[1] H Akagi. Modern Active Filters and Traditional Passive Filters. Bulletin of the Polish Academy of Sciences
Technical Sciences. 2006; 54(3): 255-269.
[2] I Habi, et al. Using the Shunt Active Power Filter for Compensation of the Distorted and Unbalanced Power System
Voltage. Proceedings of World Academy of Science, Engineering and Technology. 2006; 17: 287-291.
[3] AA Valdez, et al. An Adaptive Controller for the Shunt Active Filter Considering a Dynamic Load and the Line
Impedance. IEEE Transaction on Control Systems Technology. 2009; 17(2): 458- 464.
[4] I Colak, E Kabalci, R Bay. Review of Multilevel Voltage Source Inverter Topologies and Control Schemes. Energy
Conversion and Management. 2010; 52: 1114–1128.
[5] E Babaei, et al. Reduction of DC Voltage Sources and Switches in Asymmetrical Multilevel Converters Using a
Novel Topology. Electric Power Systems Research. 2007; 77: 1073–1085.
[6] NF Mailah, et al. Neutral-Point-Clamped Multilevel Inverter Using Space Vector Modulation. European Journal of
Scientific Research. 2009; 28(1): 82-91.
[7] S Barkati, et al. Harmonic Elimination in Diode-Clamped Multilevel Inverter Using Evolutionary Algorithms.
Electric Power Systems Research. 2008; 78: 1736-1746.
[8] ME Ortúzar, et al. Voltage-Source Active Power Filter Based on Multilevel Converter and Ultra capacitor DC Link.
IEEE Transaction on Industrial Power Electronics. 2006; 53(3): 477-485.
[9] S Saad, et al. Fuzzy Logic Controller for Three-Level Shunt Active Filter Compensating Harmonics and Reactive
Power. Electric Power Systems Research. 2009; 79: 1337–1341.
[10] A Munduate, et al. Robust Model-Following Control of a Three-Level Neutral Point Clamped Shunt Active Filter in
the Medium Voltage Range. Electrical Power and Energy Systems. 2009; 31: 577-588.
[11] G Zhou, et al. Direct Power Control of a Multilevel Inverter Based Active Power Filter. Electric Power Systems
Research. 2007; 77: 284–294.
[12] N Belhaouchet, et al. A Novel Adaptive HBCC Technique for Three-phase Shunt APF. Electric Power Systems
Research. 2009; 79: 1097–1104.
[13] M Cichowlas, et al. Active Filtering Function of Three-Phase PWM Boost Rectifier Under Different Line Voltage
Conditions. IEEE Transaction on Industrial Power Electronics. 2005; 52(2): 410-419.
[14] A Chaoui, et al. DPC Controlled Three-Phase Active Filter for Power Quality Improvement. Electrical Power and
Energy Systems. 2008; 30: 476–485.
[15] M Malinowski, et al. Simple Direct Power Control of Three-Phase PWM Rectifier Using Space-Vector Modulation
(DPC-SVM). IEEE Transaction on Industrial Power Electronics. 2004; 51(2): 447-454.
[16] BS Chen, et al. Direct Power Control of Active Filters with Averaged Switching Frequency Regulation. IEEE
Transaction on. Power Electronics. 2008; 23(6): 2729-2737.
[17] M Malinowski, et al. Virtual Flux Based Direct Power Control of Three-Phase PWM Rectifiers. IEEE Transaction
on Industry Applications. 2001; 37(4): 1019-1027.
[18] BR Lin, et al. Implementation of a three phase capacitor clamped active power filter under unbalanced condition.
IEEE Transaction on Industrial Electronics. 2006; 53(5): 1621-1630.
[19] G Zhou, et al. Direct power control of a multilevel inverter based active power filter. Electric Power Systems
Research. 2007; 77: 284-294.
[20] O Vodyakho, et al. Novel direct current space-vector control for shunt active power filters based on the three-level
inverter. IEEE Transaction on Industrial Power Electronics. 2008; 23(4): 1668-1678.
[21] M Saeedifard, et al. Analysis and Control of DC-Capacitor-Voltage-Drift Phenomenon of a Passive Front-End Five-
Level Converter. IEEE Transaction on Industrial Electronics. 2007; 54(6): 3255-3266.
[22] HA Hotait, et al. Capacitor Voltage Balancing Using Redundant States of Space Vector Modulation for Five-Level
Diode Clamped Inverters. IET Power Electronics. 2010; 3(2): 292-313.
[23] X Zhenfeng, et al. A Shunt Active Power Filter with Enhanced Dynamic performance using DualRepetitive
Controller and Predictive Compensation. International Journal of Power Electronics and Drive Systems (IJPEDS).
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Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level Three-Phase Shunt Active Power Filter

  • 1. International Journal of Power Electronics and Drive System (IJPEDS) Vol. 4, No. 2, June 2014, pp. 173~191 ISSN: 2088-8694  173 Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level Three-Phase Shunt Active Power Filter Bouzidi Mansour*,** , Bouafia Saber** , Bouzidi Ali*** , Benaissa Abdelkader** , Barkat Said**** * Department of Electronics and Communications, Faculty of New Technologies of Information and Communication University Kasdi Merbah, Ouargla, Algeria. ** Department of Electrical Engineering, Faculty of Engineering, University of Djilali Liabes, Sidi Bel Abbes, Algeria, Intelligent Control Electronic Power System laboratory (I.C.E.P.S) *** Department of Electrical Engineering, Faculty of Technology, University of Hadj Lakhdar Batna **** Department of Electrical Engineering, Faculty of Engineering, M’sila University, M’sila, Algeria. Article Info ABSTRACT Article history: Received Jan 11, 2014 Revised Mar 13, 2014 Accepted Mar 26, 2014 This paper proposes a virtual flux direct power control-space vector modulation combined with backstepping control for three-phase five-level neutral point clamped shunt active power filter. The main goal of the proposed active filtering system is to eliminate the unwanted harmonics and compensate fundamental reactive power drawn from the nonlinear loads. In this study, the voltage-balancing control of four split dc capacitors of the five-level active filter is achieved using five-level space vector modulation with balancing strategy based on the effective use of the redundant switching states of the inverter voltage vectors. The obtained results showed that, the proposed multilevel shunt active power filter with backstepping control can produce a sinusoidal supply current with low harmonic distortion and in phase with the line voltage. Keyword: Five-level shunt active power filter Direct power control Virtual flux concept Backstepping control Multilevel space vector modulation Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Bouzidi Mansour, Department of Electronics and Communications, Faculty of New Technologies of Information and Communication University Kasdi Merbah, Ouargla, 30000, Algeria Departement of Electrical Engineering, Faculty of Engineering, University of Djilali Liabes, Sidi Bel Abbes, Sidi Bel Abbes 22000, Algeria Email: bouzidi.m.28@gmail.com 1. INTRODUCTION Nowadays the power electronic equipments are widely used in distribution networks which act as nonlinear loads. Many power quality disturbances such as harmonics pollution, unbalanced load currents, and reactive power problems are caused by the nonlinear loads; as a result poor power factor, weakening efficiency, over heating of motors and transformers, malfunction of sensitive devices etc. To overcome the aforementioned problems passive filters can be used to compensate some of them. However, bulk passive components, series and parallel resonance and a fixed compensation characteristic are the main drawbacks of passive filters [1]. Therefore, to give an effective solution for harmonics concerns several active power filter (APF) topologies have been proposed. They aimed not only for current or voltage compensation but also for voltage dips, flicker and imbalance [2]. Among various active filter configurations, the shunt active power filters (SAPF) have a number of advantages [3]. Compared with the series and hybrid configurations, the SAPF do not need an additional
  • 2.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 174 coupling transformer and require much less protection and switchgear. They operate as three-phase controlled harmonic current sources and are not affected by harmonic distortions in supply voltages. In general, the ratings of shunt active power filters are based on the magnitudes of compensating current and the corresponding filter terminal voltage. For medium to high power applications the multilevel converters are the most attractive technology. Indeed, multilevel converters have shown some significant advantages over traditional two-level converters [4]-[7]. The main advantages of the multilevel converter are a smaller output voltage step, lower harmonic components, a better electromagnetic compatibility and lower switching losses [4]-[7]. In the recent time the use of multilevel inverters is prevailing in medium-voltage active power filters without using a coupling transformer [8]-[11]. Various control strategies have been proposed to control the SAPF, such as hysteresis band current control (HBCC) [12], voltage oriented control (VOC) [13]. Another interesting emerging control technique called direct power control (DPC) has been investigated [13], [14]. DPC is based on the instantaneous active and reactive power control loops. It is developed analogously with the well-known direct torque control (DTC) used for adjustable speed drives. In DPC, there are no internal current loops or modulator block because the converter switching states are selected via a switching table. Although DPC has many advantages, some disadvantages of this control technique are high ripple content in the system current, high ripple in the commanded active and reactive power, variable switching frequency, and requires a high switching frequency [15]. The DPC can be forced to operate at a constant frequency by using space vector modulation (SVM) to synthesize the space-vector voltage demanded by the switching table [15], [16]. Although classical DPC uses the fix number of vectors present in this table, more vectors can be arbitrarily generated by using SVM. In this way, the ripple in current can be reduced [15]. Recent developments have popularized the virtual flux (VF) concept, which assumes that both the grid and converter’s line filter behave as an AC motor [17]. One of the main advantages of this approach is that it is less sensitive to line-voltage variations than other approaches. The virtual flux direct power control (VFDPC) is an adaptation of the DPC to a VF reference frame [17]. In this paper, a nonlinear control strategy based on the backstepping associated to VFDPC-SVM is applied to three-phase five-level shunt power active filter in the aim to improve its performances. In the present study, it is shown via simulation results that the proposed backstepping controller has high performance both in the transient and in the steady state operations. The line currents are very close to sinusoidal waveforms, a good control of the DC-bus voltage is obtained, and unity power factor operation is achieved. 2. SHUNT APF CONFIGURATION 2.1. System Description cv av bv 4C 1aS 2aS 1 2 3 4 4Cv 1aS 2aS 3aS 4aS 3aS 4aS 1bS 2bS 1bS 3bS 4bS 3bS 4bS 1cS 2cS 1cS 2cS 3cS 4cS 3cS 4cS 0 3Cv 2Cv 1Cv 4i 3i 2i 1i 0i 2bS a b c FaiFbiFci Fau Fbu Fcu 3C 2C 1C dcv PCC 4Ci 3Ci 2Ci 1Ci FR FL FR FL FR FL sR sR sR LL sci sbi saisL sL sL LL LRLai Lbi Lci LR LR LL sce sbe sae lL lR Nonlinear Load Figure 1. Five-level shunt active power filter configuration
  • 3. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 175 The structure in Figure 1, describes the proposed SAPF based on a three-phase five-level VSC. The SAPF consists of three principal parts, the three-phase converter, four capacitors (C1, C2, C3, and C4) and the smoothing inductances LF. The converter is used to charge and to discharge the capacitors to provide the required compensating current. The capacitors are used to store energy and the inductances LF are used to smooth and decrease the ripples of the harmonic currents injected by SAPF [9]. The main task of the SAPF is to reduce harmonic currents and to ensure reactive power compensation. Ideally, the SAPF needs to generate just enough reactive and harmonic current to compensate the nonlinear load harmonic in the line. The resulting total current drawn from the AC main is sinusoidal. 2.2. Modeling of the PWM five-level inverter The topology of the three-phase five-level NPC inverter is shown also in Figure 1. Here, xv and Fxi , x = a, b, c, represent the point of common coupling (PCC) voltages and AC side currents, respectively. RF is a line resistance that models the parasitic resistive effects of the inductor LF. The capacitances of input capacitors are assume equal C1=C2=C3=C4=C. For a net dc-side voltage of vdc, each capacitor voltage is ideally vCj = vdc/4, j = 1,..., 4 and each generated phase voltage uFx, x = a, b, c, has five levels with respect to dc-side reference point 0. The switching states and the resultant phase voltages are listed in Table 1, where state conditions 1 and 0 indicate ON and OFF switch status, respectively. Table 1. Switching states of a five-level inverter Switching state 1S 2S 3S 4S 1S 2S 3S 4S Phase voltage 4 1 1 1 1 0 0 0 0 dcv 3 0 1 1 1 1 0 0 0 3 / 4dcv 2 0 0 1 1 1 1 0 0 / 2dcv 1 0 0 0 1 1 1 1 0 / 4dcv 0 0 0 0 0 1 1 1 1 0 The switching functions of the five level inverter of Figure 1, are expressed as: 4 4 3 2 1 3 4 3 2 1 2 4 3 2 1 1 4 3 2 1 0 4 3 2 1 , ou x x x x x x x x x x x x x x x x x x x x x x x x x F S S S S F S S S S F S S S S x a b c F S S S S F S S S S       (1) Referring all of the voltages to the lower DC-link voltage level (“0” reference), each output voltage consists of contributions by a determinate number of consecutive capacitors: 4 0 0 0 , , ,i j x xj C j i u F v x a b c            (2) When balanced distribution of the DC-link voltage among the capacitors is assumed: 4 0 0 , , , 4 dc x xj j v u jF x a b c    (3) The line to line voltage is given by: 0 0 0 0 0 0 ab a b bc b c ca c a u u u u u u u u u                    (4)
  • 4.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 176 The expressions of instantaneous inverter phase output voltages are given by: 1 3 Fa ab ca Fb bc ab Fc ca bc u u u u u u u u u                    (5) 2.3. Mathematical model of three-phase five levels SAPF The mathematical equations which govern the behaviour of the ac-side of shunt active filter are: 1 ( ) 1 ( ) 1 ( ) Fa Fa a F Fa F Fb Fb b F Fb F Fc Fc c F Fc F di u v R i dt L di u v R i dt L di u v R i dt L          (6) Where, , , ,Fiu i a b c represent voltages of the SAPF. By transforming (6) in stationary frames, it follows that: 1 ( ) 1 ( ) F F F F F F F F F F di u v R i dt L di u v R i dt L               (7) Where, v  and v  are the PCC voltages in the stationary α-β coordinates. Fi  and Fi  are α-β components of AC currents of SAPF. Fu  and Fu  are α-β components of AC side voltages of SAPF. The DC side of the filter can be expressed as: 1 2 3 4( )dc C C C C dv d v v v v dt dt     (8) Equation (8) can also be written as: 1 2 3 4 1 ( )dc C C C C dv i i i i dt C     (9) Where iCj ( j =1,2,3,4) is the current through capacitor Cj. The equation of DC side (9) can be related to the AC side by the following power-balance relationship: 1 1 2 2 3 3 4 4C C C C C C C C a Fa b Fb c Fcv i v i v i v i v i v i v i      (10) If we assume that the capacitor voltages are balanced, the equation (9) becomes: 1 ( )dc a Fa b Fb c Fc eq dc dv v i v i v i dt C v    (11) Where: / 4eqC C . Equation (11) can be expressed as:
  • 5. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 177 dc F eq dv p dt C  (12) Where: pF is the instantaneous active power of SAPF. F F Fp v i v i     (13) 3. NONLINEAR VIRTUAL FLUX BASED DIRECT POWER CONTROL The backstepping VFDPC-SVM control strategy main scheme is presented in Figure 2. The nonlinear load and SAPF currents are sensed using tow current sensors located in phases (a) and (b), and the estimated PCC virtual flux components ,PCC PCC   are used for the powers estimation (pL, qL and pF, qF) and backstepping power controller. PCC cv bv av F refu F refu  Lq PCC Fabci abcS Fabci Fp FqFi  Labci 3Cv 2Cv 1Cv Li  Li  Lp Frefp Frefp Lp 1Cv 2Cv C C C C Lci Lbi Lai sR sR sR LL FR FR FR FL FL FL sci sbi saisL sL sL LL LR LR LR Fai Fci Fbi LL sce sbe sae lL lR abc  4Cv 3Cv 0Frefq  abcS abc  dcv dcrefv PCC Figure 2. Backstepping VFDPC-SVM scheme of five-level SAPF The active power pL is delivered to the high pass filter (HPF) to obtain the alternate values, which finally are used as compensating component. The reactive power qL can be delivered to the HPF or directly to the input of the backstepping power controller depending on compensation requirements (compensation of higher harmonics or compensation of higher harmonics and reactive power at the same time). The reference active power pFref (generated by the outer nonlinear DC voltage controller) and reactive power reference qFref (set to zero for unity power factor) values are compared with estimated instantaneous pF and qF values augmented by their corresponding alternate load powers pL and qL, respectively. The errors are delivered to the backstepping power controller, which eliminates steady state error. The output signals from backstepping power controller are used for switching signals generation by a five-level space vector modulator [13].
  • 6.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 178 3.1. PCC virtual flux estimator The principle of VF is based on assumption that the voltages imposed by the line power in combination with the AC side inductors can be considered as quantities related to a virtual AC motor, where RF and LF represent the stator resistance and leakage inductance of the virtual motor [17]. With the definitions: PCC vdt   (14) In general RF can be neglected and the voltage v can be expressed as in stationary α- coordinates as follows: F F F F F F di v u L dt di v u L dt           (15) The integrated of both sides of (15) gives: PCC F F F PCC F F F u dt L i u dt L i               (16) The measured line currents ,F Fi i  and the estimated virtual flux components ,PCC PCC   are used for SAPF power estimation. 3.2. Active and reactive powers estimator Using the measured current and the estimated PCC virtual flux, the estimated active and reactive powers can be described by the following formulas [17]: a) Active filter powers are: ( ) ( ) F PCC F PCC F F PCC F PCC F p i i q i i                   (17) b) Nonlinear load powers are: ( ) ( ) L PCC L PCC L L PCC L PCC L p i i q i i                   (18) Where: ω is the angular frequency. Both power estimation equations are simple to calculate and do not require the computation of the current derivatives. 3.3. Active and reactive power model based on virtual flux The backstepping power controller is based on instantaneous power time derivative behavior. From Equation (17), the derivatives of active and reactive powers are given by: F PCCPCC FF F PCC F PCC PCC FPCC FF F PCC F PCC di dd didp i i dt dt dt dt dt d did didq i i dt dt dt dt dt                                         (19) For three-phase balanced system, the following relations can be written:
  • 7. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 179 , , PCC PCC PCC PCC PCC PCC v d dt dv dt                      (20) Replacing (7), (20) into (19), power derivatives can be expressed as:         PRCF F F F PRC F F PRC F F PRC F F PRCF F F F PRC F F PRC F F PRC F F dp q R i u dt L R i u L dq p R i u dt L R i u L                                              (21) 3.4. Backstepping controllers design Backstepping is a systematic and recursive design methodology for nonlinear feedback control. This approach has emerged as powerful tools for stabilizing nonlinear systems both for tracking and regulation purposes [18]. The backstepping algorithm takes advantage of the idea that certain variables can be used as virtual controls to make the original high order system simple, thus the final control outputs can be derived step by step through suitable Lyapunov functions ensuring global stability. This control method has been successfully applied on a growing collection of plant. However, few papers are devoted to the backstepping control of power electronics converters [19]-[20]. In the following, the backstepping design procedure is applied to five-level shunt active power filter. As chosen in Figure 2, the control strategy is based on a cascade structure, namely, the output of outer voltage loop is used as reference signal in the inner power loop. The approach adopted herein designs by breaking down a complex nonlinear system into smaller sub-systems, then designing control Lyapunov functions and virtual controls for these sub-systems. In order to design the control algorithm for active power filter with the aid of backstepping method, nonlinear differential Equation (12) and (21) must be portioned in three SISO subsystems at the following form: ( ); 1,2,3 k kk f k g k k k k k L h L h u y h k        (22) Where k , ku and ky represent state, control input and output of kth system, respectively. kf and kg are smooth fields, and kh is a smooth scalar function. The term kf kL h stands for the Lie derivative of kh with respect to kf , similarly kg kL h . By identifying the first subsystem, based on equation (12), with (22), it can be yield: 1 1 1 1 1 1 1 1 , , y , 0 1 dc F dc f g eq dc v u p h v L h L h C v        (23) The second and the third subsystems are built based on the active and reactive derivative (21).
  • 8.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 180 The identification of (21) with (22) leads to:           2 2 3 2 2 2 2 2 2 3 3 3 3 3 3 3 , , 1 , , 1 F F PCC F PCC F F F g f F PCC F F PCC PCC F F PCC F F F PCC F PCC F F F g f F PCC F F PCC PCC F F F p u u u u L y h p L h L h q R i R i L q u u u u L y h q L h L h p R i R i L                                                                          PCC     (24) In following sections the backstepping method will be used for developing the dc voltage and power controllers. 3.4.1. DC Voltage Controller Synthesis In order to ensure that the SAPF operates effectively it is important to maintain the dc capacitor voltage at a constant desired value. The backstepping dc voltage controller sets the active power of the inverter to regulate the dc voltage based on its reference value covering the inverter losses. The purpose of this control is to achieve the dc voltage reference, so the first tracking error is defined as: 1 1 1dz y y  (25) Where: 1d dcrefy v Differentiating (25) with respect to time, it is obtained that: 1 11 1 1 1f g Fref dz L h L h p y    (26) The candidate function of Lyapunov is chosen as: 2 1 1 1 2 V z (27) The derivative of the Lyapunov function is expressed as: 1 11 1 1 1 1 1 1( )f g Fref dV z z z L h L h p y     (28) To guarantee the Lyapunov stability, the control law is chosen as: 1 1 1 1 1 1 1 f d Fref g k z L h y p L h      (29) Where, k1 is a positive constant. 3.4.2. Power Controller Synthesis Using the backstepping approach, one can synthesize the control law forcing the active and reactive powers to follow the desired powers.
  • 9. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 181 For the first step the following tracking-errors are considered: 2 2 2 3 3 3 d d z y y z y y     (30) Where: 2 _ 3 _ d Fref total d Fref total y p y q   Where: _ _ Fref total Fref L Fref total Fref p p p q q     (31) The resulting error dynamics equation can be expressed as: 2 2 3 3 2 2 2 2 3 3 3 3 f g F ref d f g F ref d z L h L h u y z L h L h u y           (32) The chosen Lyapunov functions are given by the following expressions: 2 2 2 2 3 3 1 2 1 2 V z V z   (33) The time derivatives of Lyapunov functions 2 3andV V are given by: 2 2 3 3 2 2 2 2 2 2 2 3 3 3 3 3 3 3 ( ) ( ) f g F ref d f g F ref d V z z z L h L h u y V z z z L h L h u y               (34) In order to make negative the derivatives of Lyapunov functions, the intermediate control laws F refu  and F refu  are proposed in the following equation: 2 2 3 3 2 2 2 2 2 3 3 3 3 3 f d F ref g f d F ref g k z L h y u L h k z L h y u L h             (35) Where, k2 and k3 are positive constants. The relation between the intermediate and final control laws is given by: F ref F ref F ref F ref u u D u u                 (36) Where: PRC PRC PRC PRCF D L               
  • 10.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 182 The D matrix determinant is different to zero, so the final control laws are given as: 1F ref F ref F ref F ref u u D u u                 (37) 3.5. Space Vector Modulation with DC-Capacitor Voltages Balancing Strategy In the five-level NPC topology, the voltages of the four series-connected dc-link capacitors must be confined to vdc/4 to take advantage of the inverter. The dc-voltage backstepping control regulates only the total dc voltage. For this reason, the dc-capacitor voltages are kept equals using five-level SVPWM that takes advantages of redundant switching states to counteract the dc voltages drift phenomenon [21]. The five-level SVPWM technique can approximate the reference voltage vector, computed by backstepping power controller, using the nearest three vectors. They are selected to minimize the energy of the dc-capacitor voltages [21]. Figure 3 represents the space vector states for the five-level inverter there are 125 switching-state vectors. Applying Clark’s transformation to all combinations of output voltages associated with the 125 switching-state vectors results in 60 nonzero voltage space vectors. Projection of the vectors on αβ coordinates forms a four-layer hexagon centered at the origin of the αβ plane (Figure 3), and zero-voltage vectors are located at the origin of the plane. 1st Sector 1 1 f g Frefu m o n lj k 1 s u a b c d e h i 1 1Frefu 1 2Frefu 2 s u 400 440 410 420 430 411 300 421 310 431 320 441 330 422 311 200 432 321 210 442 331 220 433 322 211 100 443 332 221 110 000 111 222 333 444 343 232 121 010 344 233 122 011 434 323 212 101 334 223 112 001 342242 231 120 131 020 243 132 021 244 133 022 423 312 201 234 123 012 424 313 202 324 213 102 224 113 002 341241141 030 130 230 142 031 143 032 144 033 134 023 412 301 413 302 414 303 124 013 314 203 214 103 114 003 041 340240140040 042 043 044 034 024 401 402 403 404304204104004 014 2nd Sector 3rd Sector 4th Sector 5th Sector 6th Sector  F refu  F refu   1 2 1 3 1 4 1 5 1 6 1 7 1 8 1 10 1 9 1 11 1 12 1 13 1 14 1 15 1 16 Figure 3. Space voltage vectors for a five-level inverter 3.5.1. Determination of the Space Vector Location The space vector location is determined in two steps. The first step determines the sector number of where the vector lies. The second step determines the triangle in which the vector lies [22]. Step 1: Sector number computation. The reference voltage vector magnitude and its angle are determined from: 2 2 Fref F ref F refu u u   and 1 tan 2 F ref F ref u u             (38)
  • 11. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 183 Where, the tan 2-1 function returns the four-quadrant inverse tangent. Once the value of  is calculated, the sector numbers are given by [22]:  ceil 1,2,3,4,5,6 / 3 S          (39) Where ceil is the C-function that adjusts any real number to the nearest, but higher, integer. Step 2: Triangle identification. Reference vector Frefu is projected on the axes of 60° coordinate system [21]. In each sector S, the normalized projected components are 1 s Frefu and 2 s Frefu given by (40). Fig. 3 shows the projection of Frefu in the first sector. 1 2 cos( ( 1) )) sin( ( 1) ) 3 33 2 3 2 2 sin( ( 1) ) 33 2 3 2 Fref Fref S Fref dc Fref S Fref dc u u S S u v u S u v                (40) In order to identify the triangle where the required reference is located, the following integers are used:     1 1 2 2 int int S S Fref S S Fref l u l u   (41) Where the int() function returns the nearest integer that is less than or equal to its argument. The triangle number is obtained according to the value of 1 S l and 2 S l , as shown in Table 2: Table 2. Triangle identification in each sector S 1 S l 2 S l  ( 1,...,16 )S i i  0 0 16 1 2Si ( 1)S S S ref refu u   14 1 2Si ( 1)S S S ref refu u   1 0 13 1 2Si ( 2)S S S ref refu u   9 1 2Si ( 2)S S S ref refu u   2 0 8 1 2Si ( 3)S S S ref refu u   2 1 2Si ( 3)S S S ref refu u   3 0 1 S  0 1 15 1 2Si ( 2)S S S ref refu u   11 1 2Si ( 2)S S S ref refu u   1 1 10 1 2Si ( 3)S S S ref refu u   4 1 2Si ( 3)S S S ref refu u   2 1 3 S  0 2 12 1 2Si ( 3)S S S ref refu u   6 1 2Si ( 3)S S S ref refu u   1 2 5 S  0 3 7 S 
  • 12.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 184 3.5.2. Duration Time Calculation On-duration time intervals of the switching voltage vectors adjacent to the reference voltage vector Frefu of a five-level NPC are calculated as follows: s s s s s s i i i i i i s s s i i i x x y y z z Fref s x y z s u t u t u t u T t t t T                (42) Where Ts is the switching period, s i xu  , s i yu  and s i zu  are the three switching vectors adjacent to the reference voltage vector located in the triangle ( 1,...,16)s i i  formed by the vertices (x,y,z) and s i xt  , s i yt  and s i zt  are the calculated on-duration time intervals of the switching vectors, respectively. Expression (42) can by decomposed in the 60° coordinates system as follows: 1 1 1 1 2 2 2 2 s s s s s s i i i i i i s s s s s s i i i i i i s s s i i i x x y y z z Fref s x x y y z z Fref s x y z s u t u t u t u T u t u t u t u T t t t T                         (43) The coordinates of all vertices of Sth sector are given in Table 3. Table 3. Vertices coordinate in Sth sector vertices coordinates A 1 2( , ) (0,0) S S i i A Au u   B 1 2( , ) (1,0) S S i i B Bu u   C 1 2( , ) (2,0) S S i i C Cu u   D 1 2( , ) (3,0) S S i i D Du u   E 1 2( , ) (4,0) S S i i E Eu u   F 1 2( , ) (0,1) S S i i F Fu u   G 1 2( , ) (1,1) S S i i G Gu u   H 1 2( , ) (2,1) S S i i H Hu u   I 1 2( , ) (3,1) S S i i I Iu u   J 1 2( , ) (0,2) S S i i J Ju u   K 1 2( , ) (1,2) S S i i K Ku u   L 1 2( , ) (2,2) S S i i L Lu u   M 1 2( , ) (0,3) S S i i M Mu u   N 1 2( , ) (1,3) S S i i N Nu u   O 1 2( , ) (0,4) S S i i O Ou u   Substituting the coordinates of ux, uy and uz from Table 3 in (43), in each triangle, the on-duration time intervals are summarized in Table 4. These duration times are valid in all sectors. The significant outcome of the proposed algorithm is its inherent simplicity. Unlike the conventional SVM algorithm that requires solution of several sets of trigonometric equations for calculation of on-duration time intervals. Therefore, the proposed SVM algorithm is much simpler and easier for digital implementation since it reduces the hardware and software complexity and decreases the required computational time.
  • 13. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 185 Table 4. Duration time in each triangle of the Sth sector Duration time intervals Triangle S i xt S i yt S i zt 1 ( , , ) ( , , )S x y z D E I  S S i i s y zT t t     1 3S ref su T 2 S ref su T 2 ( , , ) ( , , )S x y z I H D  S S i i s y zT t t     13 S ref su T  21 S ref su T 3 ( , , ) ( , , )S x y z H I L  S S i i s y zT t t     1 2S ref su T  2 1S ref su T 4 ( , , ) ( , , )S x y z L K H  S S i i s y zT t t     12 S ref su T  22 S ref su T 5 ( , , ) ( , , )S x y z K L N  S S i i s y zT t t     1 1S ref su T  2 2S ref su T 6 ( , , ) ( , , )S x y z N M K  S S i i s y zT t t     11 S ref su T  23 S ref su T 7 ( , , ) ( , , )S x y z M N O  S S i i s y zT t t    1 S ref su T  2 3S ref su T 8 ( , , ) ( , , )S x y z C D H  S S i i s y zT t t     1 2S ref su T 2 S ref su T 9 ( , , ) ( , , )S x y z H G C  S S i i s y zT t t     12 S ref su T  21 S ref su T 10 ( , , ) ( , , )S x y z G H K  S S i i s y zT t t     1 1S ref su T  2 1S ref su T 11( , , ) ( , , )S x y z K J G  S S i i s y zT t t     11 S ref su T  22 S ref su T 12 ( , , ) ( , , )S x y z J K M  S S i i s y zT t t    1 S ref su T  2 2S ref su T 13( , , ) ( , , )S x y z B C J  S S i i s y zT t t     1 1S ref su T 2 S ref su T 14 ( , , ) ( , , )S x y z G F B  S S i i s y zT t t     11 S ref su T  21 S ref su T 15 ( , , ) ( , , )S x y z F G J  S S i i s y zT t t    1 S ref su T  2 1S ref su T 16 ( , , ) ( , , )S x y z A B F  S S i i s y zT t t    1 S ref su T 2 S ref su T 3.5.3. DC-capacitor Voltages Balancing Based on Minimum Energy Property In a five-level NPC inverter, the total energy E of dc-link capacitors is: 4 2 1 1 2 jj C j E C v    (44) When all capacitor voltages are balanced, the total energy E reaches its minimum of 2 min 8dcrefE Cv , with dcrefv is the desired value of dc voltage. This condition is called the minimum energy property which can be used as the basic principle for dc-capacitor voltages balancing and control [21]. The adopted control method should minimize a quadratic cost function J associated with voltage deviation of the dc-capacitors. The cost function is defined as follows: 24 1 1 2 4j dc C j v J C v          (45) The mathematical condition to minimize J is: 4 1 0j jC C j v i    (46) Where: / 2, 1,2,3,4Cj Cj dcv v v j   
  • 14.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 186 The capacitor currents are affected by the dc-side intermediate branch currents, i1, i2 and i3. Thus, it is advantageous to express (46) in terms of i1, i2 and i3. The dc-capacitor currents are expressed as: 3 3 1 1 , 1,2,3,4. 4j S S C x x x x j i xi i j       (47) By substituting (47) in (46), the condition to achieve voltage balancing is deduced as: 4 3 3 1 1 1 0 4j S S C x x j x x j v xi i               (48) When the DC link voltages vCj are closed to their reference vdc /4, the following condition is verified: 4 1 0jC j v    (49) Using (49), the Equation (48) can be written as: 3 3 1 0j S C x j x j v i            (50) Applying the averaging operator, over one sampling period, to (50) results in: ( 1) 3 3 1 1 0 s j s k T S C x j x js kT v i dt T                 (51) Assuming that sampling period Ts, as compared to the time interval associate with the dynamics of capacitor voltages, is adequately small, the capacitor voltages can be assumed to remain constant over one sampling period [21] and, consequently, (51) is simplified to: 3 3 1 ( ) ( ) 0j S C x j x j v k i k            (52) Where, ( )Cjv k is the voltage drift at sampling period k, and , 1,2,3ji j  is the averaged value of the ji . The current ji should be computed for different combinations of adjacent redundant switching states over a sampling period and the best combination which maximizes (52) is selected. 4. SIMULATION RESULTS The proposed backstepping controller for three-phase five-level SAPF has been simulated and compared with conventional PI controller. The parameters used are shown in Table 5. Table 5. Basic parameters of the system under study RMS value of phase voltage 5.5 kV DC-link capacitor C 5 mF Source impedance Rs, Ls 0.1 mΩ, 0.1 mH Filter impedance RF, LF 0.1 mΩ, 1 mH Switching frequency fs 4 kHz Fundamental frequency f 50 Hz DC-link voltage reference vdc ref 20 kV Diode rectifier load Rl , Ll 200 Ω, 1mH Input diode rectifier impedance RL, LL 100 mΩ, 1 mH Sampling frequency 1 MHz k1, k2, k3 constants 70, 2.105 , 2.105
  • 15. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 187 The goal of the simulation is to examine the capability of the controller to fulfill the following four different aspects. a) Harmonic current compensation b) Dynamic response performance c) Parameters variation d) Distorted grid phase voltage 4.1. Harmonic Current Compensation The AC supply current of phase (a) and its harmonic spectrums before and after compensation are illustrated in Figure 4, 5 and 6. It results that the SAPF decreases the total harmonic distortion in the supply currents from 29.68% to 2.96% with PI control and to 1.47 % with backstepping control. So, the distortion in supply current with backstepping control is less than in case of PI control method. Figure 4. (a) Supply current before harmonics compensation, (b) Its harmonic spectrum Figure 5. (a) Supply current after harmonics compensation using backstepping controller, (b) Its harmonic spectrum Figure 6. (a) Supply current after harmonics compensation using PI controller, (b) Its harmonic spectrum 4.2. Dynamic Response Performance In this section, the performances of the backstepping and PI controllers are analyzed under 100% step charge in the resistance load at t = 0.5s. 0.2 0.205 0.21 0.215 0.22 -150 -100 -50 0 50 100 150 Time (s) isa (A) (a) 0.2 0.205 0.21 0.215 0.22 -200 -100 0 100 200 Time (s) i sa (A) (a) 0.2 0.205 0.21 0.215 0.22 -200 -100 0 100 200 Time (s) i sa (A) (a)
  • 16.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 188 Figure 7. Simulation results of the proposed VFDPC-SVM using backstepping controller. (a) Source current. (b) Reduced source voltage and source current of a-phase (c) PCC active and reactive powers. (d) DC-link voltage vdc. (e) DC capacitors voltages The dynamic behavior under a step change of the load is presented in Figure 7 and 8 for backstepping and PI controllers respectively. The active power was changed stepwise from 1.7 to 3.4 MW. For clarity, a phase-a current is shown for illustration and the corresponding phase voltage is scaled down by a factor of 1/20. It can be observed that the unity power factor operation is successfully achieved, even in this transient state. As a result, the DC-bus voltage decreases, since the DC capacitors discharge. In a short time, the backstepping controller starts to respond due to the voltage error signal, which is the difference between the DC-bus reference voltage and the DC bus actual voltage. The output reference power of the controller will increase slowly to attain the required active power. When, the instantaneous value of the active power drawn from the grid is equivalent to the active power consumed by the load, the DC-bus voltage stops decreasing and the inverter stops supplying the active power. Afterwards, the DC-bus voltage returns to the value according to the DC-bus reference voltage (without overshoot with backstepping control). When the DC-bus voltage is at its reference value, the new steady state has been achieved with new grid current amplitude. From Figure 7(e), it is important to note that the application of the proposed redundant vectors based five-level SVM control maintains these voltages constant around the reference of 5kV. 0 0.2 0.4 0.6 0.8 1 -400 -200 0 200 400 Time (s) i sa (A) (a) 0.46 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54 -400 -200 0 200 400 Time (s) e a (V)andi sa (A) (b) 0 0.2 0.4 0.6 0.8 1 -1 0 1 2 3 4 5 x 10 6 Time (s) p PCC (W)andq PCC (Var) (c) 0 0.2 0.4 0.6 0.8 1 1.94 1.96 1.98 2 x 10 4 Time (s) v dc anditsreference(V) (d) 0 0.2 0.4 0.6 0.8 1 4850 4900 4950 5000 5050 5100 Times (s) Capacitorsvoltages(V) (e) v c4 v c3 v c2 v c1
  • 17. IJPEDS ISSN: 2088-8694  Application of Backstepping to the Virtual Flux Direct Power Control of Five-Level… (Bouzidi Mansour) 189 Figure 8. Simulation results of conventional VFDPC-SVM using PI controller. (a) Source current. (b) Reduced source voltage and source current of a-phase (c) PCC active and reactive powers. (d) DC-link voltage vdc. (e) DC capacitors voltages 3.3. Parameters Variation The values of the inverter-side inductors LF may vary according to the operation point and aging. A small variation in this parameter may cause erroneous virtual-flux estimation, and consequently, an incorrect amount of active and reactive powers is generated by the inverter. To show the influence of these variations in system accuracy, simulations with different inductor values are analyzed, Figure 9(a). The switching frequency is also a biasing factor on the harmonic quality of the line current as well as the size of SAPF inductances [23-24]. It is important to show its influence on the line current THD, Figure 9(b) Figure 9. Simulation results of robustness examination. (a) THD of line current versus value of SAPF inductor (b) THD of line current versus value of switching frequency. 0 0.2 0.4 0.6 0.8 1 -400 -200 0 200 400 Time (s) i sa (A) (a) 0.46 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54 -400 -200 0 200 400 Time (s) e a (V)andi sa (A) (b) 0 0.2 0.4 0.6 0.8 1 1.96 1.98 2 2.02 x 10 4 Time (s) v dc anditsreference(V) (d) 0 0.2 0.4 0.6 0.8 1 -1 0 1 2 3 4 5 x 10 6 Time (s) p PCC (W)andq PCC (Var) (c) 0 0.2 0.4 0.6 0.8 1 4900 4950 5000 5050 Time (s) Capacitorsvoltages(V) (e) v c4 v c3 v c2 v c1 1 2 3 4 5 6 7 1 2 3 4 5 6 7 L F (mH) THD(%) (a) Backstepping PI 1 2 3 4 5 6 7 8 9 10 1 2 3 4 5 6 7 Switching frequency (kHz) THD(%) (b) Backstepping controller PI controller
  • 18.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 2, June 2014 : 173 – 191 190 Figure 9(a) shows that the THD increases with the increase of the coupling inductance LF. The proposed VFDPC-SVM using backstepping controller gives the best results for all values of LF. However, for conventional VFDPC-SVM, the increase of LF leads immediately to the increase in current THD. From the Figure 9(b) one notices well that the THD decreases remarkably with increase of the switching frequency. It can be concluded that the VFDPC-SVM based on backstepping controller can be operated with reduced switching frequency (1 kHz). 3.4. Distorted Grid Phase Voltage In an ideal situation, the grid usually consists of a balanced three-phase power system with sinusoidal line voltage-waves. However, the line voltage is frequently distorted and the systems which are connected to the grid should be able to tolerate this situation. One of the main disturbances is the presence of line voltage harmonics of order 5, 7 and 11. Figure 10 shows the waveforms in which a fifth harmonic voltage component of 10% is intentionally superimposed on the fundamental grid voltage. Figure 10. Simulation results of proposed backstepping VFDPC-SVM control with distorted grid phase voltage. (a) Three-phase grid voltages. (b) PCC virtual flux. (c) Reduce source voltage and source current of a-phase. (d) Harmonic spectrum of line current. It can be observed that the grid current is nearly sinusoidal shape (THD = 3.21%) and unity power factor operation is successfully achieved even in existence of the distorted grid voltages as shown in Figure 10. This result is due to fact that voltage was replaced by virtual flux (the integrator behaves like a low-pass filter). 5. CONCLUSION This paper has investigated a virtual flux direct power control based on backstepping approach for three-phase shunt active power filter using a five-level inverter. The proposed control scheme is intended to achieve harmonics elimination, reactive power compensation, and dc voltage regulation. Simulation results show that the backstepping-based control strategy significantly reduces the current distortion to values allowed by international standards, and regulates the power factor observed in the common coupling point between the nonlinear load and the power distribution system as well as exhibits excellent transient response during large load variations. When compared to the conventional control, the backstepping control offers substantial improvements on harmonic content of supply current, and robustness to the filter parameters variations. These results confirm that the backstepping control strategy provides higher performance than the 0 0.005 0.01 0.015 0.02 -1 -0.5 0 0.5 1 x 10 4 Time (s) Threephasegridevoltages(v) (a) 0 0.005 0.01 0.015 0.02 -30 -20 -10 0 10 20 30 Time (s) VirtualfluxPCCestimation(Wb) (b) 0.285 0.29 0.295 0.3 0.305 0.31 0.315 -500 0 500 Time (s) v a (V)andi sa (A) (c)
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