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 A New Method for Determining Reference Compensating Currents of the Three-Phase Shunt Active Power Filter Gary W. Chang Author Affiliation: Depar tment of Elec tric al Engin eerin g, Na- tional Chung Cheng University, Chia-Yi, Taiwan. Abstract: Among various solutions to electric power quality prob- lems, the use of a shunt active power filter (SAPF) has been proven as an effective method to compensate reactive power and to mitigate har- mon ic cur ren ts of nonl inearloa ds.When des igninga SAPF, it is crucia l to generate reference currents for determining actual compensating current injections to the point of common coupling. In contrast to the conventional instantaneous reactive power theory that needs coordi- nat e transformations, the new met hod prop osed in this let ter is to det er- mine reference compensating currents based on the balance of the instantaneous reactive and active power generated in the SAPF. It is shown that the proposed method is suitable for reactive and harmonic power compensation by using a SAPF. In addition to maintaining the sinusoidal source currents, this method also eliminates the need for in- stalling energy storage device for reactive power compensation as well as the dc source for the harmonic compensation in the active power fil- ter. Therefore, a simpler design of the SAPF with the minimal line losses can be expected. Keywords: Activ e power filte r, refer ence compe nsati ng curre nt, instantaneous reactive power theory, coordinate transformation, in- stantaneous power balance. Introduction: The concept of using the SAPF for reactive and har- monic power compensation was introduced more than two decades ago. By measuring the load currents and voltages, the SAPF can inject compensating currents as well as absorb or generate reactive power at the point of common coupling for controlling the harmonics and com- pensating reactive power of the connected load. In 1983, Akagi et al. proposed an innovative approach based on the instantane ous reac tive power theory(i.e.,  p-q the ory)to compute SAPF reference compensating currents, and this approach inspired the devel- opment of many other p-q theor y-base d metho ds for real izing the SAPF [1], [2]. Willems indicated, however, that the p-q theory is com- plete only in three-phase systems without zero-sequence component [3]. Also, the insta ntane ous react ive power theory-based metho d re- quires coordinatetrans forma tions betwe en the a-b-c coordi nate and the  p-q coordinate, which increases the complexity when designing the SAPF controlle r. Mor e rec ent ly, Peng et al.propos ed a the ory tha t gave a gen era liz ed def inition of theinsta nta neous rea cti ve powe r in the a-b-c coordi nate [4]. Alt hough Pen g’s approach does not nee d the coordi nat e transformation, it requires an additional function for instantaneous re- active power vector calculation in the SAPF controller. Based on the instantaneous reactive power space vector defined in [4] and the con - cept of instantaneous power balance, the author of this letter presents a direct method for determining the SAPF reference compensating cur- rents. The proposed method is valid for both sinusoidal/nonsinusoidal and balanced/unbalanced three-phase power systems. Instantaneous Power Balance Method: Figure 1 shows the sche- matic diagram of a typical three-phase four-wire SAPF compensating system. The three-phase instantaneous active power consumed by the load is  IEEE Power Engineering Review, March 2001 63  Figure 1. The schematic diagram of the three-phase SAPF compensation  Figure 2. Source voltage, source currents before and after compensation at each phase ( v  k  , i lk  , i  sk  , k a b c = , , )
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 A New Method for Determining ReferenceCompensating Currents of the Three-PhaseShunt Active Power Filter 

Gary W. Chang

Author Affiliation: Department of Electrical Engineering, Na-tional Chung Cheng University, Chia-Yi, Taiwan.

Abstract: Among various solutions to electric power quality prob-lems, the use of a shunt active power filter (SAPF) has been proven asan effective method to compensate reactive power and to mitigate har-monic currents of nonlinear loads.When designing a SAPF, it is crucialto generate reference currents for determining actual compensatingcurrent injections to the point of common coupling. In contrast to theconventional instantaneous reactive power theory that needs coordi-nate transformations, the new method proposed in this letter is to deter-mine reference compensating currents based on the balance of theinstantaneous reactive and active power generated in the SAPF. It isshown that the proposed method is suitable for reactive and harmonicpower compensation by using a SAPF. In addition to maintaining thesinusoidal source currents, this method also eliminates the need for in-stalling energy storage device for reactive power compensation as wellas the dc source for the harmonic compensation in the active power fil-ter. Therefore, a simpler design of the SAPF with the minimal linelosses can be expected.

Keywords: Active power filter, reference compensating current,instantaneous reactive power theory, coordinate transformation, in-stantaneous power balance.

Introduction: The concept of using the SAPF for reactive and har-monic power compensation was introduced more than two decadesago. By measuring the load currents and voltages, the SAPF can injectcompensating currents as well as absorb or generate reactive power atthe point of common coupling for controlling the harmonics and com-pensating reactive power of the connected load.

In 1983, Akagi et al. proposed an innovative approach based on theinstantaneous reactive power theory (i.e., p-q theory)to compute SAPFreference compensating currents, and this approach inspired the devel-opment of many other p-q theory-based methods for realizing theSAPF [1], [2]. Willems indicated, however, that the p-q theory is com-plete only in three-phase systems without zero-sequence component

[3]. Also, the instantaneous reactive power theory-based method re-quires coordinate transformations between the a-b-c coordinate and the

 p-q coordinate, which increases the complexity when designing theSAPF controller. More recently, Peng et al.proposed a theory that gavea generalized definition of theinstantaneous reactive power in the a-b-ccoordinate [4]. Although Peng’s approach does not need the coordinatetransformation, it requires an additional function for instantaneous re-

active power vector calculation in the SAPF controller. Based on theinstantaneous reactive power space vector defined in [4] and the con-cept of instantaneous power balance, the author of this letter presents adirect method for determining the SAPF reference compensating cur-rents. The proposed method is valid for both sinusoidal/nonsinusoidaland balanced/unbalanced three-phase power systems.

Instantaneous Power Balance Method: Figure 1 shows the sche-matic diagram of a typical three-phase four-wire SAPF compensatingsystem. The three-phase instantaneous active power consumed by theload is

 IEEE Power Engineering Review, March 2001 63

 Figure 1. The schematic diagram of the three-phase SAPF compensation Figure 2. Source voltage, source currents before and after compensation ateach phase ( v

 k , i

lk , i

 sk , k a b c= , , )

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 p t v t i t v t i t v t i t l a la b lb c lc( ) ( ) ( ) ( ) ( ) ( ) ( )= + + . (1)

The three-phase instantaneous reactive power vector, ql, defined in [4],

can be expressed as

q

a b c

v v v

i i i

l a b c

la lb lc

=

(2)

or

( ) ( ) ( )q v i v i a v i v i b v i v i cl b lc c lb c la a lc a lb b la= − + − + −

, (3)

where the magnitude of the three-phase instantaneous reactive powerin each phase becomes

qv v

i ila

b c

lb lc

= ,

qv v

i ilb

c a

lc la

=

,

qv v

i ilc

a b

la lb

=

.

(4)

In (4), the instantaneous reactive power at one phase represents thepower transferred between the other two phases without a contributionto the active power delivered from the source to the load. As shown inFigure1, the instantaneous active and reactive powers delivered to anonlinear load must satisfy (5) and (6):

 p t p t p t p t p t l s f l lh( ) ( ) ( ) ( ) ( )= + = +1 , (5)

q t q t k a b c fk lk ( ) ( ), , ,= = (6)

where p sand p f 

are instantaneous active power supplied by the sourceand the SAPF, and where pl 1 and plh

are instantaneous active funda-mentaland harmonic power of theload. q fk  is the instantaneous reactivepower generated by the SAPF at phase k .

As shown in Figure 1, in order to ensure a fundamentalactive powersupplied to the load from the source, the instantaneous reactive powerand harmonic components of active power must be compensated by theSAPF. Assume that the SAPF is lossless, the source side contains onlysinusoidal fundamental current with a unity power factor when the bal-ance of instantaneous power at the SAPF is maintained.

Reactive Power Compensation: According to (4) and (6), the in-

stantaneous reactive power to be compensated by the SAPF at eachphase can be expressed by

q

q

q

v v

v v

v v

i

i

 fa

 fb

 fc

c b

c a

b a

 fa

 fb

=−

−−

0

0

0 i

q

q

q fc

la

lb

lc

=

.

(7)

It should be noted that the coefficient matrix in (7) has a rank of two.Therefore, the active power current injections required for instanta-neous reactive power compensation can not be determined directlyfrom (7). Since the instantaneous active power required from the SAPFfor reactive power compensation is zero, thefollowing relation holds:

 p v i v i v i f a fa b fb c fc= + + = 0. (8)

After solving (7) and (8) simultaneously, the SAPF reference compen-sating currents become

i ip

v v vv k a b c fk lk 

l

a b c

k = −+ +

=2 2 2

, , , .(9)

Thesecond term in (9) implies that theactive power current componentis supplied by the source and the SAPF only compensates the reactivepower component of the load current.

Harmonic and Reactive Power Compensation: When consider-ing compensation of both of harmonic power and reactive power, (8)becomes

 p v i v i v i p f a fa b fb c fc lh

= + + = . (10)

From (7) and (10), the SAPF compensating currents are determined tobe

i ip

v v vv

p

v v vv

ip

v

 fk lk l

a b c

k lh

a b c

lk l

a

= −+ +

++ +

= −

2 2 2 2 2 2

1

2 2 2+ +=

v vv k a b c

b c

k , , , .

(11)

Similar to (9), the second term on the right of (11) can be interpretedas the fundamental active power component of the load current sup-plied by thesource. Therefore, theSAPF compensates both thereactive

64 IEEE Power Engineering Review, March 2001

 Figure 3. SAPF reference compensating current at phase a ( i fa

 )

 Figure 4. Instantaneous and average active power supplied by the SAPF dur-ing compensation

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