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74 CHAPTER 4 INSTANTANEOUS SYMMETRICAL COMPONENT THEORY 4.1 INTRODUCTION This chapter deals with instantaneous symmetrical components theory for current and voltage compensation. The technique was introduced by Fortescue. It is applied to resolve an unbalanced three-phase system of voltages and currents into three balanced systems of voltages and currents. The operation of control circuit is explained using analytical computations. The steady state and dynamic operation of control circuit in different load current and/or utility voltages conditions is studied through simulation results. It does not need phase lock loop or complicate computations. The analytical analysis and simulation results are presented to study the operation of control circuit in dynamic and steady state cases. The symmetrical component theory originally defined for steady-state analysis of three phase unbalanced systems. A three-phase four-wire distribution system supplying an unbalanced and nonlinear load is considered for simulation study. The detailed simulation results using MATLAB are presented to support the proposed compensation strategy. 4.2 COMPUTATION OF REFERENCE CURRENT The effectiveness of an active power filter depends basically on the design characteristics of the current controller, the method implemented to generate the reference template and the modulation technique used. The

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Page 1: chapter 4 instantaneous symmetrical component theory

74

CHAPTER 4

INSTANTANEOUS SYMMETRICAL

COMPONENT THEORY

4.1 INTRODUCTION

This chapter deals with instantaneous symmetrical components

theory for current and voltage compensation. The technique was introduced

by Fortescue. It is applied to resolve an unbalanced three-phase system of

voltages and currents into three balanced systems of voltages and currents.

The operation of control circuit is explained using analytical computations.

The steady state and dynamic operation of control circuit in different load

current and/or utility voltages conditions is studied through simulation results.

It does not need phase lock loop or complicate computations.

The analytical analysis and simulation results are presented to study

the operation of control circuit in dynamic and steady state cases. The

symmetrical component theory originally defined for steady-state analysis of

three phase unbalanced systems. A three-phase four-wire distribution system

supplying an unbalanced and nonlinear load is considered for simulation

study. The detailed simulation results using MATLAB are presented to

support the proposed compensation strategy.

4.2 COMPUTATION OF REFERENCE CURRENT

The effectiveness of an active power filter depends basically on the

design characteristics of the current controller, the method implemented to

generate the reference template and the modulation technique used. The

Page 2: chapter 4 instantaneous symmetrical component theory

75

icc

iln

S1 S3

ilb

ilc

ila

iln

ilc

CdcLf,R f

Linear/Non-Linear

Loadsisc

S5

S6 S2S4

icaicb

DSTATCOM

ilailb

Vdc

3-Phase4-Wire AC

Mains

icn

isa

isb

iln

+-

+-

control scheme of a shunt active power filter must calculate the current

reference waveform for each phase of the inverter, maintain the dc voltage

constant, and generate the inverter gating signals. Also the compensation

effectiveness of an active power filter depends on its ability to follow the

reference signal calculated to compensate the distorted load current with a

minimum error and time delay.

Figure 4.1 Schematic diagram of shunt active power filter

Active filters are widely employed in distribution system to reduce

the harmonics. Various topologies of active filters have been proposed for

harmonic mitigation. The schematic diagram of shunt active power filter

topology is shown in Figure 4.1. The shunt active power filter based on

Voltage Source Inverter (VSI) structure is an attractive solution to harmonic

current problems. The shunt active filter is a PWM voltage source inverter

that is connected in parallel with the load. Active filter injects harmonic

current into the AC system with the same amplitude but with opposite phase

as that of the load. The principal components of the APF are the VSI, DC

energy storage device, coupling inductance and the associated control circuits.

Page 3: chapter 4 instantaneous symmetrical component theory

76

The power system is configured with four wires. The AC source is

connected to a set of non-linear loads. Voltages Vsa, Vsb,Vsc and current Ila, Ilb,

Ilc indicate the phase voltages and currents at the load side respectively. Iln is

the neutral current of the load side. The APF consists of three principal parts,

a three phase full bridge voltage source inverter, a DC side capacitor and the

coupling inductance Lf. The capacitor is used to store energy and the

inductance is used to reduce the ripple present in the harmonic current

injected by the active power filter. The shunt active filter generates the

compensating currents to compensate the load currents Ila, Ilb, Ilc so as to

make the current drawn from the source (Isa, Isb, Isc) as sinusoidal and

balanced. The performance of the active filter mainly depends on the

technique used to compute the reference current and the control system used

to inject the desired compensation current into the line. In this chapter, the

instantaneous symmetrical components theory is used to determine the current

references (Ifa*, Ifb*, Ifc*).

The primary goals of DSTATCOM are to cancel the effect of poor

load power factor such that the current drawn from the source has a near unity

power factor and to cancel the effect of harmonic contents in loads such that

the current drawn from the source is nearly sinusoidal. In addition, it can also

eliminate dc offset in loads.

The reference current for DSTATCOM is calculated by

instantaneous symmetrical component theory. It is assumed that source

voltages are balanced and are given by

)120tsin(v

)120tsin(v

tsinv

sc

sb

sa

(4.1)

Page 4: chapter 4 instantaneous symmetrical component theory

77

The symmetrical component theory originally defined for steady

state analysis of 3-phase unbalanced systems. This transformation is the result

of multiplying the transformation matrix by the phasor representation of

unbalanced 3-phase system.

A=

1 1 121 a a

21 a a

(4.2)

where, 32j

ea

sc

sb

sa

2

231

2

1

0

VVV

aa1aa1111

VVV

(4.3)

The V0 , V1 and V2 stand for phasor presentation of zero, positive

and negative sequence components of phase-neutral voltage in the phase “a”,

respectively. The Vsa , Vsb and Vsc stands for phasor presentation of voltages

of phases a, b and c, respectively. The first part of control strategy of shunt

active filter is based on computing of instantaneous positive sequence of load

side currents and utility side voltages using instantaneous symmetrical

component theory.

The objective of compensation is to provide balanced supply

current such that zero sequence component is zero. We therefore have

i 0scisbisa (4.4)

This guarantees that zero sequence current flowing through the

neutral is zero in a three phase four wire system.

Page 5: chapter 4 instantaneous symmetrical component theory

78

va2vav3

1v scsbsa1sa

(4.5)

The angle of the vector is then given by

v

vv

vvv

vvv

sa

sb sc1

scsbsa

scsb11sa

23

23

21

21

23

23

tantan

(4.6)

If we now assume that the phase of the vector isa1 lags that of vsa1 by

an angle , we get

iaiivavav sc2

sbsasc2

sbsa a (4.7)

Substituting the values of a and a2 ,Equation (4.7) can be expanded as

)()()()( iiiiivvvvv scsbscsbsascsbscsbsa 23j

21

21

23j

21

21

(4.8)

Equating the angles, we can write from the above equation

4k3k

2k1k 11 tantan (4.9)

where

vv sbsa231k

,)( vvv scsbsa 2

1212k

ii sbsa233k

,)( iii scsbsa 2

1214k

Page 6: chapter 4 instantaneous symmetrical component theory

79

Using the formula

tantantantantan(

1

Equation (4.9) can be expanded as

tan

tan)(tan tan

4k3k14k

3k

4k3k

2k1k 1

(4.10)

Solving the above equation we get

0333

ivvvivvvivvv

scscsbsasbsbsasc

sasascsb

(4.11)

where

3tan

(4.12)

When the power factor angle is assumed to be zero, Equation (4.12)

implies that the instantaneous reactive power supplied by the source is zero.

On the other hand, when this angle is non-zero, the source supplies a reactive

power that is equal to times the instantaneous power.

The instantaneous power in a balanced three-phase circuit is

constant while for an unbalanced circuit it has a double frequency component

in addition to a dc value. In addition, the presence of harmonics adds to the

oscillating component of the instantaneous power .The objective of the

compensator is to supply the oscillating component such that the source

supplies the average value of the load power. Therefore,

piviviv lavscscsbsbsasa (4.13)

Page 7: chapter 4 instantaneous symmetrical component theory

80

where plav is the average power drawn by the load. Since the harmonic

component in the load does not require any real power, the source only

supplies the real power required by the load. Combining equations (4.4),

(4.11) and (4.13),

piii

vvvvvvvvvvvv

lavsc

sb

sa

scsbsa

scsbsasbsascsascsb 00

333111

(4.14)

Assuming that the current are tracked without error, the Kirchoffs

current law(KCL) at PCC can be written in terms of the reference currents as,

iii sklkfk (4.15)

where k=a, b, c.

Substituting the above equation in Equation (4.14) and solving

pvvv

vvvii

pvvv

vvvii

pvvv

vvvii

lav2sc

2sb

2sa

sbsasclcfc

lav2sc

2sb

2sa

sascsblbfb

lav2sc

2sb

2sa

scsbsalafa

(4.16)

By using these Equation (4.16), reference compensator currents are

calculated.

4.3 MODELING OF SHUNT ACTIVE FILTER

From the schematic diagram of compensated system given in

Figure 4.1.

Page 8: chapter 4 instantaneous symmetrical component theory

81

The loop equation for phase ‘a’(Upper loop) is,

faf f fa sa c1diL +R i +v -v =0dt

fa sa c1ffa

f f f

di v vR=- i - +dt L L L (4.17)

The loop equation for phase ‘a’(Lower loop) is,

di R vvfa sa c2f=- i - -dt L L Lfaf f f (4.18)

-di R v vvfa sa c1 c2f=- i - + S -Saadt L L L Lfaf f f f (4.19)

-di vR v vfb sb c1 c2f=- i - + S -Sbdt L L L Lfb bf f f f (4.20)

-di R v vvfc sc c1 c3f=- i - + S -Sccdt L L L Lfcf f f f (4.21)

Capacitor Currents i1 and i2 is given by,

1

dvc1C = -i = - S i +S i +S ia cdt fa b fb fc (4.22)

2

- - -dvc1C = i S i +S i +S ia b cdt fa fb fc (4.23)

Then defining a state vector of the state space equation is given as,

Tx = i i i v vc1 c2fa fb fc (4.24)

Page 9: chapter 4 instantaneous symmetrical component theory

82

Combining the Equations (4.19) to (4.23), we get,

d/dt

fa

fb

fc

c1

c2

iiivv

=

-

a af

f f f

-

b bf

f f f-

c cf

f f f

a b c

- - -

a b c

SR S- 0 0 -L L L

SR S0 - 0 -L L L

SR S0 0 - -L L L

S S S- - - 0 0C C C

S S S 0 0C C C

fa

fb

fc

c1

c2

iiivv

+f

f

f

1- 0 0L10 - 0L

10 0 - L

sa

sb

sc

vvv

(4.25)

4.3.1 Switching Control of DSTATCOM

The shunt component of UPQC can be controlled in two ways,

a) Tracking the shunt converter reference current, when the shunt

converter current is used as feedback control variable. The

load current is sensed and the shunt compensator reference

current is calculated from it. The reference current is

determined by calculating the active fundamental component

of the load current and subtracting it from the load current.

This control technique involves both the shunt active filter and

load current measurements.

b) Tracking the supply current, when the supply current is used

as the feedback variable. In this case the shunt active filter

ensures that the supply reference current is tracked. Thus, the

supply reference current is calculated rather than the current

injected by the shunt active filter. The supply current is often

required to be sinusoidal and in phase with the supply voltage.

Page 10: chapter 4 instantaneous symmetrical component theory

83

Since the waveform and phase of the supply current is known, only

its amplitude needs to be determined. Also, when used with a hysteresis

current controller, this control technique involves only the supply current

measurement. Thus, this is a simpler to implement method. Therefore it has

been used in the UPQC simulation model.

4.3.2 DC Voltage Control Using PI Controller

In Figure 4.1, assume S and S1 are the status of the switch in top

and bottom half of an inverter leg. The switch status, S=1 and S1=0 implies

that the top switch of the inverter leg is closed and it connects the inverter leg

to Vc1=Vdc while the bottom switch in the same leg is open. Similarly for S=0

and S1=1, the bottom switch connects the inverter leg to Vc2= -Vdc and the

top switch in the inverter leg is open. Therefore, through the inverter

switching arrangements the inverter supplies a voltage + Vdc. We now have to

choose the control signal S=1 or 0 and S1=0 or 1, such that appropriate

inverter connection is achieved. DC voltage control using PI controller is

shown in Figure 4.2.Any deviation of the capacitor voltage from the reference

is due to losses. The PI controller loops draws the loss from the ac system to

hold the voltage constant.

Figure 4.2 DC voltage control using PI controller

Page 11: chapter 4 instantaneous symmetrical component theory

84

Different current control techniques are applied for tracking the

reference current. They are sampled error control, hysteresis band control,

sliding mode controller, linear quadratic regulator, deadbeat controller and

pole shift controller. From the number of current-control techniques, the

hysteresis control appears to be the most preferable for shunt active filter

applications. Therefore, in the UPQC simulation model a hysteresis controller

has been used. The advantages of using a hysteresis controller are simpler

implementation, enhanced system stability, increased reliability and response

speed.

In hysteresis control, the controlled current is monitored and is

forced to track the reference within the hysteresis band. The inverter switches

are made to change their states at instances when the controlled current

touches the upper or lower limit of the hysteresis band. The controlled current

is forced to decrease when it reaches the upper limit and to increase when it

reaches the lower limit.

By alternately reversing the polarity of the dc capacitor the

controlled current is forced to alternately increase or decrease within the

hysteresis band following the reference current. The narrower the hysteresis

band (smaller values of h) the more accurate is the tracking, but this also

results in higher switching frequency.

If the current references are assumed to be composed from zero

sequence components, the line currents will return through the ac neutral

wire.In the “split capacitor” inverter topology, the current of each phase to

flow either through or through and to return through the ac neutral wire. The

currents can flow in both directions through the switches and capacitors.

Page 12: chapter 4 instantaneous symmetrical component theory

85

When rises and decreases, but not with equal ratio because the

positive and negative values are different and depend on the instantaneous

values of the ac phase voltages. The inverse occurs when the dc voltage

variation depends also on the shape of the current reference and the hysteresis

bandwidth. Therefore, the total dc voltage, as well as the voltage difference

will oscillate not only at the switching frequency, but also at the

corresponding frequency of that is being generated by the VSI. The switches

are controlled asynchronously to ramp the current through the inductor up and

down so that it follows the reference.

When the current through the inductor exceeds the upper hysteresis

limit a negative voltage is applied by the inverter to the inductor. This causes

the current in the inductor to decrease. Once the current reaches the lower

hysteresis limit a positive voltage is applied by the inverter to the inductor and

this causes the current to increase and the cycle repeats.

If a dynamic offset level is added to both limits of the Hysteresis

band, it is possible to control the capacitor voltage difference and to keep it

within an acceptable tolerance margin. Normally 5 % of the load current is

taken as Hysteresis-band width. Hysteresis current controller derives the

switching signals of the inverter power switches (IGBTs). The current

controllers of the three phases are designed to operate independently. Each

current controller determines the switching signals to its inverter bridge. The

switching logic for phase a,b and c is formulated as follows.

For Phase a:

If ifa > (ifa* + hb) then upper switch is OFF & lower switch is ON.

If ifa < (ifa* - hb) then upper switch is ON & lower switch is OFF.

Page 13: chapter 4 instantaneous symmetrical component theory

86

For Phase b:

If ifb > (ifb* + hb) then upper switch is OFF & lower switch is ONIf ifb < (ifb * - hb) then upper switch is ON & lower switch is OFF

For Phase c:

If ifc > (ifc* + hb) then upper switch is OFF & lower switch is ONIf ifc < (ifc * - hb) then upper switch is ON & lower switch is OFF

where ‘hb’ is the width of the hysteresis band around the reference current.

4.4 COMPUTATION OF REFERENCE VOLTAGE

The series component of UPQC is controlled to inject the

appropriate voltage between the point of common coupling (PCC) and load,

such that the load voltages become balanced, distortion free and have the

desired magnitude. Theoretically the injected voltages can be of any arbitrary

magnitude and angle. However, the power flow and device rating are

important issues that have to be considered when determining the magnitude

and the angle of the injected voltage. Figure 4.3 shows schematic diagram of

a series-compensated distribution system.

In UPQC-Q the injected voltage is maintained 90 degree in advance

with respect to the supply current, so that the series compensator consumes no

active power in steady state. In second case UPQC-P the injected voltage is in

phase with both the supply voltage and current, so that the series compensator

consumes only the active power, which is delivered by the shunt compensator

through the dc link.

Page 14: chapter 4 instantaneous symmetrical component theory

87

In the case of quadrature voltage injection UPQC-Q the series

compensator requires additional capacity, while the shunt compensator VA

rating is reduced as the active power consumption of the series compensator is

minimised and it also compensates for a part of the load reactive power

demand. In UPQC-P, the series compensator does not compensate for any

part of the reactive power demand of the load, and it has to be entirely

compensated by the shunt compensator. Also the shunt compensator must

provide the active power injected by the series compensator. Thus, in this case

the VA rating of the shunt compensator increases. The reference voltage for

DVR is calculated by using instantaneous symmetrical component theory.

Figure 4.3 Schematic diagram of a series-compensated distribution system

Let the source voltages in phase a,b and c are represented by Vsa,

Vsb and Vsc. The source is connected to the DVR by a feeder with an

AFSh

Zsa

isaThree-PhaseThree-WireNonlinear

Loads

vsc

Zsb

isbZsc

isc

vsa

vsb

Cd

Cr

Lr

CrLr Lr

Cr

Page 15: chapter 4 instantaneous symmetrical component theory

88

impedance of R+jX. The DVR is represented by voltage sources vfa, vfb and vfc.

Using Kirchoffs voltage law at PCC we get,

lft VVV (4.26)

where vl is the load voltage, vt is the voltage at the PCC, and vf is the voltage

injected by the series filter. The instantaneous symmetrical components for isa,

isb and isc are defined as,

sc

sb

sa

a

a

a

a

iii

aaaa

iii

i2

23

1

2

1

0

012

11

111

(4.27)

For balanced currents the component ia0 is equal to zero,and the

component ia1 is complex conjugate of ia2. The same transformation is applied

for voltages.

The main aim of the DVR is to make the load voltage a strictly

positive sequence. Furthermore, the DVR must not supply or absorb any real

power. To force vl to be positive sequence vf must cancel the zero-and

negative-sequence components of vt. Here the DVR must operate in zero

power mode,

sctcsbtbsatatavlav IVIVIVPP (4.28)

where ptav is the average value of the instantaneous power entering the

terminal and plav is the instantaneous power supplied to the load.

Equation (4.28) can be rewritten as,

211200 aaaaaa ivivivp (4.29)

Page 16: chapter 4 instantaneous symmetrical component theory

89

Since the desired load voltages are balanced sinusoids and the

currents flowing through the series compensator are also balanced

(shunt compensator action), the instantaneous UPQC output power is constant

and this must be equal to the average power entering the UPQC (losses are

neglected).

Let us denote the phasor load voltage as

1lV V (4.30)

Since the load voltage is strictly positive sequence, the average

power to the load is also positive sequence. Therefore,

1 1 cos( )lav lP V I (4.31)

Therefore,

2*211

*1

*0

*0 ,, tftftf VVVVVVV (4.32)

An inverse symmetrical component transformation of above

equation produces the reference phasor voltages of the DVR. The

instantaneous phase voltages then can be obtained from the phasor voltages.

Once the instantaneous load voltages are obtained, the reference series filter

voltages are obtained using the following expression,

tlf VVV (4.33)

In the case when the UPQC-P control strategy is applied, the

injected voltage is in phase with the supply voltage. Hence, the load voltage is

in phase with the supply voltage and there is no need for calculating the angle

of the reference load voltage. Thus, the reference load voltage is determined

by multiplying the reference magnitude (which is constant) with the

sinusoidal template phase-locked to the supply voltage. Then, the reference

series filter voltage is obtained using the Equation (4.33).

Page 17: chapter 4 instantaneous symmetrical component theory

90

Comparing the techniques for calculating the reference voltage of

the series compensator, presented above, it can be concluded that the UPQC-P

algorithm has the simplest implementation (it involves very little

computation). In the UPQC-P case the voltage rating of the series

compensator is considerably reduced. Also, the UPQC-Q compensation

technique does not work in the case when the load is purely resistive.

Therefore, the UPQC-P control strategy has been used in the UPQC

simulation model.

4.5 MODELING OF SERIES ACTIVE FILTER

The basic purpose of the DVR is to inject a set of three phase

voltages such that the voltage vl at the critical load terminal is balanced with a

pre-specified magnitude and phase angle.

Figure 4.4 Single-phase equivalent circuit of DVR

Page 18: chapter 4 instantaneous symmetrical component theory

91

Let this voltage be denoted by vl, then applying Kirchoffs Voltage

Law(KVL), the DVR reference voltage vk is given by

tlk VVV (4.34)

Once the reference voltage is generated, it is tracked in a Hysteresis

band state feedback control. Consider the DVR single-phase equivalent circuit

shown in Figure 4.4. In this Figure, the inverter output voltage is represented

by the dc voltage (vdc) times the switching function u =1. Also, the

transformer leakage inductance is denoted by Ld and Rd represents the

switching losses.

Defining the system state vector as Tx = v ik d, the state space

equation of the system is,

.x =Ax+Bu +Dic l2 (4.35)

where, uc is the continuous-time equivalent of u and

10 CkA= Rd1- -L Ld d

0vB= dc- Ld

1- CD= k0

(4.36)

4.5.1 Switching Control of DVR

In the state feedback control, uc is given by

u =-K x-xc ref (4.37)

Page 19: chapter 4 instantaneous symmetrical component theory

92

where, K is the feedback gain matrix and xref contains the references of the

state vector. The inverter switching logic is then

If uc >h, then u=+1,

If uc <h, then u=-1,

where, h is a small positive constant that defines the Hysteresis band.

4.6 MODELING OF UPQC

The equivalent circuit of the UPQC compensated system is shown

in Figure 4.5. The inductance Lf represents the leakage inductance of the

shunt transformer and similarly the inductance Ld is the leakage inductance of

the series transformer.

Figure 4.5 Equivalent circuit of the UPQC compensated system

The switching losses of an inverter and the copper loss of the

connecting transformer are represented by a resistance Rf and Rd. The iron

losses of the transformer are neglected. The load is assumed to be an RL load

Page 20: chapter 4 instantaneous symmetrical component theory

93

characterized by R1 and L1. The voltage sources Vdc1 and Vdc2 are the voltage

Vdc across the d.c. storage capacitor multiplied by the switch function of the

shunt and series inverters respectively. The purpose of UPQC control is to

determine these switch functions.

Let us define the following state vector,

1 2 3 4 t dTx = i i i i v v (4.38)

The state-space equation of the circuit then can be written as,

UBVBAxx S 21 (4.39)

1

1 1

1 1 1

2 2

10 0 0 0

10 0 0 0

10 0 0 0

10 0 0 0

1 1 1 0 0 0

1 10 0 0 0

RL

f

f f

d

d d

LR

L LR

L LAR

L L

C C C

C C

1 2

0 01

00

0 000 00

0 000 0

dc

f

dc

d

VLL

B BV

L

11

22

1 dc

dcdc

Vuu

Vu V (4.40)

Page 21: chapter 4 instantaneous symmetrical component theory

94

In general the control variables are injected current if, inserted

voltage vd, the terminal voltage vt along with the two capacitor currents.

Furthermore, the presence of the load current in the state variable feedback is

undesirable as the load may change at any time. We must therefore perform a

suitable state transformation such that all the pertinent signals appear as state

variables. One suitable transformation is given by

1

2

1 0 1 0 0 01 1 1 0 0 00 0 0 0 1 01 0 0 0 0 00 0 1 1 0 00 0 0 0 0 1

f

c

s

s

c

d

iiv

ziiv

(4.41)

The state equation can be transformed into,

UPBVPBZPAPZ S 211 (4.42)

4.6.1 Switching control of UPQC

Assuming that we have full control over u, an infinite time Linear

Quadratic Regulator(LQR) is designed. The control law is defined as,

u = -K(z-zref) (4.43)

where zref is the desired state vector.

The control signal computed so far using the LQR is a continuous

signal. In practice the control signal u is the switching decision of the VSI of

the UPQC and is thus constrained to be + 1. The switching is then based on

u = -hys(K(Z-Zref)) (4.44)

Page 22: chapter 4 instantaneous symmetrical component theory

95

Here the hys function is defined for a small limit around zero.

If u >lim then hys(u)=1

Else if u <lim then hys(u)=-1

The selection of lim determines the switching frequency while

tracking the reference. This switching control gives good convergence to the

tracking band as well as good stability of tracking.

4.6.2 Voltage Control of the DC Bus

For a voltage source inverter the dc voltage needs to be maintained

at a certain level to ensure the dc-ac power transfer. Because of the switching

and other power losses inside UPQC, the voltage level of the dc capacitor will

be reduced if it is not compensated. Thus, the dc link voltage control unit is

meant to keep the average dc bus voltage constant and equal to a given

reference value. The dc link voltage control is achieved by adjusting the small

amount of real power absorbed by the shunt inverter. This small amount of

real power is adjusted by changing the amplitude of the fundamental

component of the reference current. The ac source provides some active

current to recharge the dc capacitor. Thus, in addition to reactive and

harmonic components, the reference current of the shunt active filter has to

contain some amount of active current as compensating current. This active

compensating current flowing through the shunt active filter regulates the dc

capacitor voltage.

Usually a PI controller is used for determining the magnitude of

this compensating current from the error between the average voltage across

the dc capacitor and the reference voltage. The PI controller estimates the Ploss

component and determines the duty cycle of the chopper to maintain the

Page 23: chapter 4 instantaneous symmetrical component theory

96

capacitor voltage at a prespecified set reference voltage. The PI controller has

a simple structure and fast response. Thus, a PI controller has been used for dc

link voltage control in the UPQC simulation model. The set values are taken

approximately 1.3 times the peak AC voltage of the source voltage for

compensator to work satisfactorily.

4.7 SIMULATION RESULTS

This section presents the details of the simulation carried out to

demonstrate the effectiveness of the proposed control strategy for the active

filter for harmonic current filtering, reactive power compensation, load

current balancing, load voltage compensation and neutral current elimination.

In the proposed work, the reference compensator currents and voltages are

generated using the instantaneous symmetrical component theory to achieve

the load current compensation and reactive power compensation. The

switching control of the voltage source inverter based on hysteresis current

controller used in the DSTATCOM and DVR is presented. The switching

harmonics due to the VSI of the DSTATCOM and DVR are eliminated. The

simulation results before and after the compensation is presented.

The test system consists of a three phase supply connected to a set

of non-linear loads namely, a 3-phase diode-bridge rectifier with RL load.

The values of the circuit elements used in the simulation are given in

Table 4.1. The simulation was conducted under unbalanced distorted source

conditions. The comprehensive simulation results are presented below.

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Table 4.1 System parameters of UPQC

System parameters Specifications

System frequency 50 Hz

Dc link capacitance C1=4400 F,C2=4400 F

Dc-link voltage 600V

Non-Linear Load R =20 ohms,

L=15 mH,

2.6 KVA

Shunt Inverter Filter L=5.5 mH ,

C=12 µF

Series Inverter Filter L=5.5 mH ,

C=12 µF

Switching Frequency 9730 Hz

PWM Control Hysteresis control

Coupling transformer 3.3 KVA

4.7.1 Compensation of current harmonics

Figure 4.6 shows the simulation results of the system with the

proposed approach. Figure.4.6 (a) shows the waveforms of the source

voltages before compensation. The source voltage is intentionally assumed to

be much distorted with 7th harmonic and 13th harmonics to better show the

behavior of the active filter under severe conditions. The Total harmonic

Distortion (THD) of the distorted three-phase load voltages are 41.51%,

35.17% and 40.36% respectively. Figure.4.6 (b) shows the waveforms of the

load voltages before compensation Figure.4.6(c) shows the waveforms of the

load voltages after compensation using series active filter .

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The THD of load voltages in phase A, B and C has reduced to

5.98%, 5.17% and 5.86 % respectively. After the installation of the UPQC,

the three phase load voltage is balanced and sinusoidal and it is in phase with

the supply voltage. The resulting THD, showing the successful performance

of the proposed control approach. The reached THD is sufficiently close to

the acceptable level suggested by IEEE-519 standards.

Figure. 4.6 (a) Source Voltages before Compensation

Figure. 4.6 (b) Load Voltages before Compensation

Figure 4.6 (c) Load Voltages after Compensation with UPQC

4.7.2 Compensation of Load Voltage

Figure.4.7(a) shows the waveforms of the load currents before

compensation using shunt active filter. In this case the simplest control system

that is a hysteresis controller for the shunt compensator is used. There is a

hysteresis controlled Inverter in each phase accompanied by a High Pass

Filter (HPF) to suppress the high frequency ripples introduced by the inverter.

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Figure. 4.7(b) shows the Compensating current of shunt active

filter. Figure.4.7(c) shows the waveforms of the source currents after

compensation using shunt active filter The THD of the distorted three-phase

line currents (Ia, Ib & Ic ) are 37.35%, 28.12% and 33.74% respectively. The

THD of current in phase A, B and C has reduced to 5.12%, 4.66% and 4.98%

respectively. The reached THD is sufficiently close to the acceptable level

suggested by IEEE-519 standards.

Figure 4.7 (a) Load current before Compensation

Figure 4.7 (b) Compensating current

Figure 4.7 (c) Source current after Compensation

After the installation of the UPQC, the three phase source current is

balanced and sinusoidal and it is in phase with the supply voltage. Source

delivers constant real power and zero reactive power to the load which

indicates that the source side power factor is maintained at unity.

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4.8 CONCLUSION

A new control strategy for UPQC is presented. This method is easy

to implement and it has reasonable dynamic response. The control strategy

generates reference compensating currents of shunt active filter and reference

compensating voltages of series active filter in such a manner that the source

side currents and load side voltages become sinusoidal and balanced in

various power quality conditions. The analytical expressions and simulation

results explain the circuit operation and the validity of presented method.