SVM Based Hysteresis Current Controller for a Three Phase Active Power Filter
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Transcript of SVM Based Hysteresis Current Controller for a Three Phase Active Power Filter
8/19/2019 SVM Based Hysteresis Current Controller for a Three Phase Active Power Filter
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National Power
Energy
Conference
(PECon) 2004
Proceedings, Kuala
Lumpur,
Malaysia
132
SVM
Based
Hysteresis Current Controller for a
Three Phase Active Power Filter
L.
P.
Ling,
and
N
A.
Azli
Absfract-a space vector modulation
(SVM)
based *hysteresis
current controller
(HCC)
technique for a three phase shunt active
power filter is proposed. The switching control algorithms of the
proposed SVM based HCC manage to generate compensated
curre nt according to
the
reference current. Harmonics extraction
is
based
on
the instantaneous active and reactive power theorem
in t ime
domain
by
calcutating
t h e
power compensation.
A
closed
loop
control system is implemented and the error current
is
the
difference between
the
reference curren t obtained from the power
compensation and the actual current
that
needs
to be
injected
back into the line.
By
iniplementing this
control
strategy, the
active power filter
(APF)
manages
' t o
generate better
compensated harmonics curren ts
t o
the line.
I n d u
Terms-Active pow er filter, Com pens ated
harmonics
current, Hysteresis current controller, Instantaneous reactive
power, R eactive power com pensation, Space vector m odulation.
I. INTRODUCTION
S
power electronics are widely used nowadays, these
A oads seems to be the
most
common source
of
power
harmonics in the power system Passive and active power
filters
APF)
re used
in
order
to
improve this unclean power
supply. Different techniques and control strategies for
APFs
had been proposed depending on the conditioning purpose
required. Various conditioning methodologies of active power
line conditioning had been discussed
in
111.
Besides that, there
are various types
of
active power filter's configurations. The
common categories of APFs are shunt, series and hybrid
configurations. However, shunt APFs are
mostly used
in
the
commercial stage. It
i s
normally a voltage fed inverter
wth
a
current
minor
loop
[2], [3].
There are many control strategies
for
shunt APFs.
One popular
time
dom ain analysis tool is
the
instantaneous power theorem (pq theorem) by
Akagi et al.
in
1980s.
This theorem depen ds
on the instantaneous
current and
voltage.
This
theorem is applied
in
conjunction
wt a PWM
current controller
in
order
to
produce appropriate switching
signals for the harmonics current compensator
t41-163.
The
hysteresis current controller
(HCC)
is the
most
commonly
proposed control method
in
time
domain. This
method
provides instantaneous current corrective response, good
h o w
Pei Ling
is with
the Control
and
Instrumentation Engineering
Department, Faculty of Electrical Engineering, Univmih Tehologi
Malaysia,
81310
UTM Skudai, Malaysia (e-mail: [email protected]).
Naziha
Ahmad Azli is with the
Energy
Conversion Department
(ENCON), Faculty
of Electrical Engineering, Universiti Telolologi Malaysia,
81 3 IO
URVl Skudai, Malaysia
(e-mail:[email protected]).
0-7803-8724-4/04/ 20.0002004
IEEE.
accuracy and unconditioned stability to the system. Besides
that, this technique
is
the easiest and most suitable for current
controlled inverters
[l],
[ 7 ] ,
[SI.
The disadvantage of
this HCC
is
that
it
requires high switching frequency, However,
this
weakness, can be overcome by conjunction
of
the space vector
modulation (SVM) technique to the controller. SVM was
first
introduced by the German researchers in the mid of 1980s.
This
technique showed several advantages aver the traditional
pulse width modulation
fPWM)
technique.
S V M
technique
can maximize the output voltage and also reduce
the
switching
number at the same carrier frequency
of
the PWM method.
Besides
that, it can
be
easily programmed and implemented
in
digital system
[91-[12].
This
paper presents the analysis based on the combination
of
the three techniques above. The conjunction
of
the S V M
technique
wth
the HCC
generates gate switchmg pulses
for
the APF and the instantaneous active and reactive power
theory
@q
theorem)
is
used
to
generate the reference
compensated current
for
the current controller
as
this system is
implemented
in
a closed
loop
form. The three phase shunt
APF
generates
the
desired com pensated
harmonics
currents for each
phase according to the error between the reference current
from the pq
theorem and
the
generated compensated current
from
the shunt
APF.
'
11. S YS T E M
CONFIGURATION
Fig.
1
shows the fimdaniental blocks
of
the proposed closed
loop
control
strategy for a three phase
APF. The
configuration
for
the APF
is
in
the f o rm
of
a current regulated voltage source
inverter. Power compensation technique
in
conjunction
wt
the SVM based HCC is
used
to generate appropriate gate
switching signals
for the
three
phase APF.
Reactive power compensation technique is used to isolate
the desired compensated harmonics
it*
with the fundamental
signal. The desired compensated harmonics
i,
is used as the
reference current
in
the
system This
allows the proposed
APF
to
produce
the
output current according to the reference
current i,
from
the pq calculation. Besides that, the feedback
current signal is the output current
i of
the
inverter whch
needs
to
be injected back
into
the power line.
The current
error signal is
acquired
from
the difference
between the reference current and the feedback current. This
current error signal is then fed
into two
sets
of
hysteresis
comparators
to
determine
the
region and the vector
of
the
reference current.
The
status
of the
outer and inner ban d errors
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133
are sent into
the
region detector and
the
switching function
table. Six sets of appropriate gate switching signals are
generated and are sent
to
the voltage source inverter. The
desired compensated current is generated by the three phase
inverter and i s injected back into each power line
to
compensate the distorted Lines current.
The transformation coordinates of the related space vectors
are
shown as follows:
1 -0.5
-0 .5
‘:,“ 1 -
Fig.
1
Block diagram
of
the proposed
APF
As a
result, he conventional pow er for thee phase circuits
be derived as follows:
’
= - - - -,
. -k e p . p =
e
+ epip
(3)
and the instantaneous reactive power is defined as follows:
(4)
- - -
= Fa x p+ ep x ia
=
evia -ea’,
From (3) and (4), the equation can be expressed as
5)
can
A
Reactive power
compensalion
The instantaneous active and reactive power theory deals
with the voltages and currents mathematically to calculate the
imaginary power
of
the three phase power circuits. The
instantaneous imaginary power
is
the reactive power which
needs
to
be
eliminated.
This
pq theorem performs
and
from S) ,
the instantaneous compensating currents can be
derived
by
6 )
instantaneously
as
the calculation
is
based
on
th
nstantaneous
voltages and currents
of
the three phase circuits
[4].
The instantaneous voltages,
e,, eb ,e,
,
and
currents, ,
b
,
aS
the
compensator will only compensate the instantaneous
reactive power,
the
real power
is
always
set to zero. The
instantaneous reactive power is set into opposite vectors in
iC
I
are
expressed as instantaneous ’pace Fig’
shows
order to cancel the
the transfomutions Of the
three phase
and
component in the line current, The
t h e e
phase
compensated currents are defined
as follows:
vectors in
~ 4 - c
oordinates
into
orthogonal coordinates,
coordinates.
i
(7)
These instantaneous compensating currents
for
each phase
icn*,
icb*,
and
ice*
are
used as
the
reference currents for
the
current
Fig. 2.
Orthogonal coordinate transformation
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134
controller.
3
S
VM Bused HCC
The S V M echnique treats the inverter as a whole unit,
which
is different when compared to P W M echnique. The
inverter
can
be driven to one of the eight unique switching
states, where each state corresponds to
a
space vector
[lo],
[12].
Fig.
3
shows
the space voltage vectors according
to
the
eight switching states.
Vo is
the
zero
voltage vector,
and
it
normally has
two
switching pattems
Vo (000) and V,
(1
11).
However,
in this
paper, the zero voltage vector is always set
to
vo (000).
v4 (011)
I
v3
010)
v2 (1
IO)
Fig.
3.
Space vectors and derivative vectors
of
current
error
in
region
I
The derivative vectors deidt
o f
the current error determines
the correct or deslred space voltage vectors
VI: or
each state.
Fig,
3
shows the desired output space voltage vectors
V,*
is
located in region I. The derivative vectors of the current error
respect to
the
output space.voltage vector
in
region
I
shows
that del/dt and de2/dt provides the mini values
of
derivative
vectors of
t h e
current
error. Hence, the correct
space voltage vectors
for V,*
are
V,,
Vz and Vo.
Based
on the
SVM
principles,
o n l y
correct and adequate
vectors
will be
applied
in
each switching state.
By
implementing this
technique
to the HCC, this
can reduce the
unnecessary number of switching. HCC is used to denote
further information
of
the derivative vectors
of
the current
error.
Two
sets
of
different tolerance band hysteresis
comparators
are
used. Each
set
consists
of
three individual
hysteresis comparators. The wider tolerance band hysteresis
comparator
is called the outer
band
controller
which is
used to
denote the region
of the
output vectors. And the comparator
wth
narrow
band
or
the inner band comparator
is
used to
denote the proper sp ace voltage vectors. The
output signais of
the outer band
HCC,
Bo Bb
B
aad the
output
signals
of
the
inner band
HCC, BairBbi Bci,
provides
the
information to a
programmable logic array to produce appropriate gate
switching signals
to the
three phase APF.
The
signals
of
each sets
of
the hysteresis comparator fo r all
regions are arranged
in
Table 1
to show
the output
of
the
desired space vectors
Vk and the
related
regions of
each state.
To
avoid confusion, each
Vk of
each state is represented
by
three
output
parameters,
y l
y2 and y3
w h c h a re
set
according
to the output signals of the inner
band hysteresis comparators.
These three parameters are then used to generate
gate switching signals of
the
APF.
TABLE
I
SVM BASED WITCHINGUNCTIONAELE
six sets
of
111 SIMULATION RESULTS
The
performance of the proposed control strategy
is
evaluated
through
digital simulation using Matlab Simulink
program.
The
outer tolerance bands and
the inner
tolerance
bands are set to roughly 8 and
4
of the maximum
harmonics current respectively. However, as the applied loads
are dynamic,
the
settings
of
the tolerance band have to be
reconsidered.
This is
because the magnitudes
of
the
harmonics
current are changing according to
t h e
loads applied.
Fig. 4(a) shows
the
compensated
harmonics current in
phase
A
which
is
injected
to
the
line by the
APF with the
outer
and inner bands tuned to
3.0
and 1.2A respectively.
T h s
tolerance bands are tuned in
wt
respect to the initial
harmonics loads
current. These bands produced
smooth
and
fine compensated harmonics current for the whole simulation
of
dynamics
loads. Fig.
4(b)
and (c) shows a wider range
of
tolerance bands settings for outer and inner bands. However,
the outputs obtained are not satisfactory. Wider tolerance
bands failed to produce accurate output signals for
the SVM
switching function table.
Fig.
5(a) shows
the
distorted
line
current
of
dynamic
load's change
in
phase A. The
desired com pensated harmonics
current
due
to the changing loads is
shown
in
Fig.
5(b).
This
compensated harmonics current is regenerated and injected
back
into
the
line by the
SVM
based
HCC
active power filter.
Fig.
5(c ) shows
the compensated supply current
of
phase
A
wth dynamically changing oads. Analysis
of
10cycles
of
the
signals
in Fig. 5 shows
that the proposed APF reduces the
THD
of the supply line current
from 30.11
to 5.32% which
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135
the comparison of the harmonics spectrum for uncompensated
and compensated fine currents'are shown inFig. 6 .
C o m m s a l e d Harmonics Currenl
- ~ . 1 3
0.t35
0.14 0.145 0.15
0.155 0.18 0,185
(al
IiamonIcs Spectrum br the Uncmpensaled Line
Currenl
Fundament4 ( 5M Z) = 210.7, THO= 30.11%
t I
8 83;
I
(a)
Hannmic$Spectmmbr the Compensated Line
Current
Fundamental 50Hr)=
210.5,
M O = 5.32%
Fig.
6.
Ilarmonics spectrum
(a)
distorted line current,
(b) compensated line current.
(E)
l l m e
8)
Fig. 4.
Compensated
harmonics
current with outer and inner
Loleraiice bands are
set
to
(a)
3.0 and 1.2
A
respectively,
(b) 6.4 and
3.2
A respectively, (c ) 14.4 and
7.0 A
respectively.
Thc
sccond
niost
sigtiificant hannotiics uf h c distorted linc
current which is about 20 of the fundamental component
is
reduced to 4% of the fundamental component. As a result, the
THD
o f
the line current is improved.
r
0 05 0.l
(a)
0.15
0.2
300,
0.05
0.1 b)
0.15
0.2
0.1
(cl
0.15
0.2
T i m i i s
Fig.
5 . Current
waveform
(a) distorted
line
current,
(b)
Compensated harm onics current, (c) Compensated
suppIy
current.
IV . CONCLUSlON
The
proposed APF has managed to produce compensated
harmonics
current regardless to the changing
of
loads. The
SVM
based HCC has provided proper switching vectors tu the
APF
by
detecting the region and vectors of each states. Better
compensated harmonics current is obtained by setting snialler
tolerance bands for the hysteresis comparators.
v.
REFERENCES
W. M . rady, M
Samotyi,
and A. H
Noyola, Survey of
active line
conditioning methodologies;' f6E.E
Transnclions
011 Power D d i i w y
H Akagi, ''Trends
in
active power line conditioners, IEEE
TransacIiorrs on Power Electronics, vu]. 9 pp.
263-268,
ay 1994.
H. Akagi, New trends
in active
fi l ters
for
power conditioning,
IKEE
ransactions on
Industry Applicarions, vol.
32,
pp. 1312-1322,
Nov/Dcc 1936.
H. Akagi.
Y.
Kanewa, and A. Nabae. Instantaneous reactive power
compensators comprosing switching devices without energy storage
components,
IEEE Pans .
Indus l ry Applications.
vol.lA-20,
pp. 625-
630, May/June 1984.
F. 2
Peng,
H. Akagi, rnd
A. Nabae, A Novel
Harmonics Power
Filter.
IEEE Transactions Power Electronicr Specinlisfs Conference, PGSC
8 8
Record, pp. 1151-1 159, 11 -14 ApriI 1988.
M. redes,
and
L
F.
C. Monteira, A control slratcgy for shunt active
filter, presented at the 10
ln temat ional
Conrerence: llarmonics and
Quality of Power, vol . 2, pp.
4 7 2 4 7 7 ,
2002.
vol. 5, pp.1536-1542, July 1990.
8/19/2019 SVM Based Hysteresis Current Controller for a Three Phase Active Power Filter
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David M.
E.
Ingram, and S. D. Round, “A
novel
digital hysteresis
current controller for
s n
active power filter,” in
f r o c .
1997
international Conlerence
on
Power Electronics
and
Drive Sysfems,
May 26-29, vol. 2, pp.
IEEE
744-749.
S . Buso,
S.Fasolo,
and
I-.
Malesani, “A dead-beat adaptive hysteresis
current control,” IEEE Transactions on
Industry
Applicofions, vot. 36,
pp, 1174-1180, uly/August
2000.
M.
P. Kazmierkowski, M. A. Dzieniakowski, and W ulkowski, ‘Wove1
Space vector based current controllers for
PWM-Inverters,”
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Jan
1991.
[lo] B. H.
Kwon, T. W
Kim. and
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H
Youm,
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VI. BIOGRAPHIES
Leow l’ei Ling
was born in
the
state of Selangor in
Malaysia, on August 5*, 1980. She paduated from
Universiti
Teknologi
Malaysia
in
the year of 2003.
She is currentiy
undergoing her
master’s degree in
electrical engineering majoring in Mechatmnics and
Automation Control in the Faculty
of
Electrical
Engineering, Univeniti Teknologi Malaysia.
Naziha
Ahmnd Arli has
been serving for 16
years as
a lecrurer at the Faculty
of
Electrjcal
Engineering,
Universiti
Teknologi
Malaysia.
She
received
h r
l3.Sc.E.E. degree from the University of Miami,
Florida,
U S A
and her M.E.E. and Ph.D degrees from
Universiti
Teknologi
Malaysia in 1986, 1992 and
2002 respectively. She currently teaches power
electronics at both undergraduate and
masters level.
Her research interests include pow er converters
sta t ic
applications,
power quality and PVifuei
cell power
systems.