Design of Grid Connected Three-phase Inverter … of Grid Connected Three-phase Inverter with Series...

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Design of Grid Connected Three-phase Inverter with Series Resonant Filter and Reduced Control over Synchronization and Real and Reactive Power Injection Daming Zhang and Eliathamby Ambikairajah University of New South Wales, Sydney, Australia Email: [email protected] AbstractThis paper investigates an inverter-topology with a series connected resonant filter for its integration with the existing power grid. It is found that such an inverter demands less control, yet it still effectively fulfills synchronization with an injection of pre-set real and reactive power into the grid. It can meet harmonics standards requirement with moderate amount of power injection into the grid. A windowed-sinc low-pass filter is introduced to extract the fundamental component of inverter terminal voltages for quick synchronization with the grid voltage and connecting the inverter to grid with the closing of circuit breaker. Index Termsgrid-tie inverter, harmonics, resonant filter, synchronization I. INTRODUCTION There has been intensive research on grid-tied inverters, due to the booming of renewable energy generation[1-3]. Such inverters need to contain several basic control units including grid synchronization, current control and harmonics injection minimization[4-6]. There have been voltage source inverter (VSI) topologies based on LCL filters, and active filters etc, each of which needs complicated control algorithms. There has also been research on harmonic mitigation techniques [4-7]. In this paper, the authors introduce a simple, yet effective, inverter topology and its control algorithm that meets synchronization requirements, and mitigates harmonics injection requirement and real and reactive power injection requirement. Such a control algorithm is modified from the synchronous d-q frame based PQ closed-loop voltage oriented control and it does not need information of the impedance of the power grid with which it is connected. Synchronization and connection of the inverter with the power grid is an important step in renewable energy applications [8-9]. In this paper, the authors introduce a windowed-sinc low-pass filter that can effectively extract the fundamental component of the output voltage at the inverter terminals, which is then compared with the Manuscript received October 4 2012; revised November 30, 2012. voltage at the point of common coupling (PCC) for paralleling the inverter generation with the power grid[7- 11]. It is found that such a filter is very effective in the proposed application. This paper is organized as follows: In Section II, the single-phase topology of the inverter with series resonant filter is presented and its performance is studied in detail; Section III presents the overall system under study, containing grid connected three-phase inverter with series resonant filter, windowed-sinc filter design, and the results and discussion; Section IV concludes the paper. II. PERFORMANCE OF SERIES RESONANT FILTER FOR VSI BASED INVERTER Fig. 1 shows a single-phase series resonant filter for VSI inverter. To study the performance of such filter, one can build Eqns. (1) and (2). Then one can discretize them into (3) and (4). By using the iteration method, one can study the performance of the series-connected resonant filter. For the normal grid, the equivalent impedance at point of common coupling (PCC) is quite small. Hence when designing the LC resonant filter, one can choose a proper reactance 1/( ) L C at power frequency. At higher frequencies, L becomes larger and 1/( ) C smaller. Provided that L becomes large enough at the third-order harmonic compared with equivalent source impedance Z L , the 1/( ) L C can share almost all harmonic voltage produced by the VSI based inverter. By doing so, the harmonic voltage injection into the system is contained. L C Z L + _ PWM () v t + + _ _ L () v t C () v t + _ () Load v t Figure 1. Series-connected resonant filter PWM () () () () C di t v t L v t Ri t dt (1) International Journal of Electrical Energy, Vol.1, No.1, March 2013 12 ©2013 Engineering and Technology Publishing doi: 10.12720/ijoee.1.1.12-17

Transcript of Design of Grid Connected Three-phase Inverter … of Grid Connected Three-phase Inverter with Series...

Page 1: Design of Grid Connected Three-phase Inverter … of Grid Connected Three-phase Inverter with Series Resonant Filter and Reduced Control over Synchronization and Real and Reactive

Design of Grid Connected Three-phase Inverter

with Series Resonant Filter and Reduced Control

over Synchronization and Real and Reactive

Power Injection

Daming Zhang and Eliathamby Ambikairajah University of New South Wales, Sydney, Australia

Email: [email protected]

Abstract—This paper investigates an inverter-topology with

a series connected resonant filter for its integration with the

existing power grid. It is found that such an inverter

demands less control, yet it still effectively fulfills

synchronization with an injection of pre-set real and

reactive power into the grid. It can meet harmonics

standards requirement with moderate amount of power

injection into the grid. A windowed-sinc low-pass filter is

introduced to extract the fundamental component of

inverter terminal voltages for quick synchronization with

the grid voltage and connecting the inverter to grid with the

closing of circuit breaker.

Index Terms—grid-tie inverter, harmonics, resonant filter,

synchronization

I. INTRODUCTION

There has been intensive research on grid-tied inverters,

due to the booming of renewable energy generation[1-3].

Such inverters need to contain several basic control units

including grid synchronization, current control and

harmonics injection minimization[4-6]. There have been

voltage source inverter (VSI) topologies based on LCL

filters, and active filters etc, each of which needs

complicated control algorithms. There has also been

research on harmonic mitigation techniques [4-7]. In this

paper, the authors introduce a simple, yet effective,

inverter topology and its control algorithm that meets

synchronization requirements, and mitigates harmonics

injection requirement and real and reactive power

injection requirement. Such a control algorithm is

modified from the synchronous d-q frame based PQ

closed-loop voltage oriented control and it does not need

information of the impedance of the power grid with

which it is connected.

Synchronization and connection of the inverter with

the power grid is an important step in renewable energy

applications [8-9]. In this paper, the authors introduce a

windowed-sinc low-pass filter that can effectively extract

the fundamental component of the output voltage at the

inverter terminals, which is then compared with the

Manuscript received October 4 2012; revised November 30, 2012.

voltage at the point of common coupling (PCC) for

paralleling the inverter generation with the power grid[7-

11]. It is found that such a filter is very effective in the

proposed application.

This paper is organized as follows: In Section II, the

single-phase topology of the inverter with series resonant

filter is presented and its performance is studied in detail;

Section III presents the overall system under study,

containing grid connected three-phase inverter with series

resonant filter, windowed-sinc filter design, and the

results and discussion; Section IV concludes the paper.

II. PERFORMANCE OF SERIES RESONANT FILTER FOR

VSI BASED INVERTER

Fig. 1 shows a single-phase series resonant filter for

VSI inverter. To study the performance of such filter, one

can build Eqns. (1) and (2). Then one can discretize them

into (3) and (4). By using the iteration method, one can

study the performance of the series-connected resonant

filter. For the normal grid, the equivalent impedance at

point of common coupling (PCC) is quite small. Hence

when designing the LC resonant filter, one can choose a

proper reactance 1/ ( )L C at power frequency. At

higher frequencies, L becomes larger and

1/ ( )C smaller. Provided that L becomes large enough

at the third-order harmonic compared with equivalent

source impedance ZL, the 1/ ( )L C can share almost

all harmonic voltage produced by the VSI based inverter.

By doing so, the harmonic voltage injection into the

system is contained.

L CZL

+

_

PWM ( )v t

+ + __L ( )v t C ( )v t

+

_

( )Loadv t

Figure 1. Series-connected resonant filter

PWM

( )( ) ( ) ( )C

di tv t L v t Ri t

dt (1)

International Journal of Electrical Energy, Vol.1, No.1, March 2013

12©2013 Engineering and Technology Publishingdoi: 10.12720/ijoee.1.1.12-17

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C( )( )

dv ti t C

dt

(2)

PWM1 ( ) ( ) ( ) / ( )Ci j t v j v j Ri j L i j

(3)

C C( ) ( ) / ( 1)v j i j t C v j (4)

In a current control based VSI inverter, the chosen

inductance or capacitance has influence on harmonic

components of the injected current. For the constant

power control, the equivalent load seen by the inverter

can be modeled by an impedance. If one assumes that

only real power P is injected into grid, then the equivalent

load impedance of the inverter is a resistor. Given the real

power injected into grid and voltage at PCC, one can use 2 /PCCV P to compute the equivalent resistance seen by the

inverter.

In the following study, inductance is set equal to 30mH

and capacitance 337.74µF.

Fig. 2 shows the PWM voltage PWM( )v t for the study

of harmonics across the equivalent load calculated

by2 /PCCV P . Fig. 3 and 4 are the results with equivalent

load resistance of 20Ω. The total harmonic distortion is

12.19%. Fig. 5 and 6 are the results with load resistance

of 2Ω. The total harmonic distortion is 1.22%. One can

see that such a series-resonant-filter based VSI inverter

topology is very suitable for the application of a large

amount of power generation under which the harmonics

requirement set by standard, can be satisfied with a small

inductance value. To supply low power into grid, the

required inductance is high in order to meet this

harmonics requirement.

Figure 2. PWM voltage PWM ( )v t

.

Fig. 7 shows the relationship between total harmonic

distortion (THD) and power injected into power grid,

from which one can see that for a given inverter system

with fixed parameters of inductance and capacitance, the

THD decreases with the increase of power injection into

grid. With the increase in inductance and corresponding

decrease in capacitance, the THD decreases. Hence, it

allows such a system to be used for smaller power

injection conditions, yet it still meets the THD

requirement. If one considers the bulkiness of the

inductor, then one can see that an inverter with a series

resonant filter is the most suitable for high power

applications such as above 25kW renewable generation,

in which the required inductance is less than 10mH and

THD can be satisfied with a significant margin.

Figure 3. Voltages across inductor, capacitor and load for a load resistance of 20 Ω.

Figure 4. Harmonics of source voltage and load voltage for a load

resistance of 20 Ω.

Figure 5. Voltages across inductor, capacitor and load for a load resistance of 2 Ω.

Figure 6. Harmonics of source voltage and load voltage for a load resistance of 2 Ω.

Figure 7. THD against power injected into grid with (1) L=10mH and C=1013.2 µF; (2) L=30mH and C=337.74 µF; (3) L=90mH and

C=112.58µF.

III. THREE-PHASE VSI INVERTER WITH SERIES-

CONNECTED RESONANT FILTER

The overall system of the three-phase inverter with

series-connected resonant filter is shown in Fig. 8. In the

system, there is one three-phase load, which consumes

International Journal of Electrical Energy, Vol.1, No.1, March 2013

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10kW real power and 0VAr reactive power. The source

internal impedance is very small and it is set as a swing

source. Between the source and point of common

coupling (PCC) there is a line impedance in each phase,

each being formed by a 0.2Ω resistor in series with a

3mH inductor. Initially, the breaker is in the open

position. The synchronisation algorithm is implemented,

as described later in this paper.

DC Three-phaseInverter

PCC

Three-phaseload

Resonant fitler

Co

nn

ecti

on

im

ped

ance

Breaker

Three-phasesource

Figure 8. Overall inverter system under study.

Fig. 9 an illustrates that the grid voltage at PCC is

taken as the reference signal, and reference voltages

gdv and gqv are computed. Figure 9b shows that the three-

phase currents out of inverter are measured and converted

into i and i then converted into di and qi .

di and qi are

compared with their respective reference signals *

di and

*

qi , which are obtained by (6) with targeted real and

reactive power injection into the grid. The differences

between *

di and di , and

*

qi and qi are fed into a simple

controller: proportionality controller. The outputs from

the controller are added with gdv and gqv references. Next

v and v are obtained and converted into three-phase

reference voltages. These reference voltages are

compared with a 1kHz triangular waveform. Finally, six

gate signals are produced to control the inverter.

*

* 2 2

1 gd gqd

gq gdq gd gq

v v Pi

v vi Qv v

(6)

gv

abc

PLL

je

f

gV

gdv

gqv

(a)

abc

+_

je , ,a b ci

i

i

+_

di

qi

*

di

*

qi

KP

KP

++

++

gdv

gqv

je

vabc

v

*v

(b)

1s

2s

X

X

Breaker command

Breaker command

Figure 9. Computation of reference voltage for gating signal

generation.

Initially the breaker is in the open position. The

breaker command sent to it is set to zero. The

synchronisation algorithm is implemented to synchronize

PCC voltage and inverter output voltage. 1s

and 2s in

Fig.9b are as follows:

*

1 ( ) BreakerCgd p d ds v k i i

(7)

*

2 ( ) BreakerCgq p q qs v k i i

(8)

Where BreakerC=0 before synchronization and

BreakerC=1 after the breaker is closed or the system is

synchronized.

Hence before circuit breaker is closed,

1 gds v (9)

2 gqs v (10)

By doing so, the inverter voltage is attempting to

follow the voltage at PCC after the system is powered up.

After the circuit breaker is closed,

*

1 ( )gd p d ds v k i i (11)

*

2 ( )gq p q qs v k i i (12)

Then control of power injection into the grid is

fulfilled after the breaker is closed.

To make an effective synchronization, in the authors’

work, a windowed-sinc low pass filter is introduced to

extract the fundamental component of inverter terminal

voltages. Three-phase voltage sensors are installed at the

output of the inverter. Outputs from the sensors are then

fed into the controller where the windowed-sinc filter is

part of it.

The kernel of the windowed-sinc filter is given

below[9]

sin 2 ( / 2)( ) [0.42

/ 2

0.5cos(2 / ) 0.08cos(4 / )

cf i Mh i K

i M

i M i M

(13)

Where fc is the cutoff frequency, expressed as a fraction

of the sampling rate, a value between 0 and 0.5. The

sample number kernel is determined by M, which must be

an even integer. The sample number i is an integer that

runs from 0 to M, resulting in M+1 total points in the

filter kernel. The constant K is chosen to provide unity

gain at zero frequency. To avoid a divide-by-zero error,

for i=M/2, use h(i)=2πfcK.

In our modeling, the sample frequency is 50kHz.

Hence the designed windowed-sinc filter has the kernel

as shown in Fig.10.

Figure 10. The kernel of the windowed-sinc filter with a sample rate of

50kHz.

International Journal of Electrical Energy, Vol.1, No.1, March 2013

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This windowed-sinc low-pass filter performs well for

signals with no DC bias. The output voltages from the

inverter contain a lot of harmonic components but they do

not have a DC component. Hence the chosen windowed-

sinc low-pass filter suits in this case, and can effectively

and quickly extract the fundamental components of the

inverter voltage.

Initially the breakers are in the open position. The

control algorithm controls the inverter to synchronize the

output voltage of the inverter with those of the grid. The

following algorithm is implemented to judge whether

synchronization has been reached:

2( ) /ra a gaE v v m

(14)

2( ) /rb b gbE v v m

(15)

2( ) /rc c gcE v v m

(16)

where av ,

bv and cv are the fundamental components

of the output voltages at inverter terminals extracted by

the windowed-sinc filter and gav , gbv and gcv are the

three-phase grid voltages and m is the number of points

per cycle. The summation is for one-cycle data.

Only when all three errors are less than pre-set values,

the breaker is closed. The synchronization and paralleling

of the inverter with the power grid through the closure of

the breaker take a short time, around 0.04s, as can be seen

in Fig. 11.

Fig. 11, 12 and 13 show the inverter currents, load

currents and source currents. From Fig. 11, one can see

that the currents injected into the grid produce an almost

sinusoidal waveform with minor distortion, whose

harmonic components are shown in Fig. 14, from which it

can be seen that the harmonic component is almost

negligible. Fig. 12 is the three-phase load current. The

three-phase load is set as unity power factor load. Hence,

it does not absorb reactive power. The reactive power

from the inverter is injected into the grid and balanced by

the source. Since the set real power is 20kW and reactive

power is -10kVAr by the inverter and load real power

consumption is 10kW, the extra 10kW real power from

inverter and reactive power from it are pumped into

source. Fig. 13 is the current into the source that

facilitates these real and reactive powers flowing into the

source.

Fig. 15 is the calculated reference voltages vgd and vgq,

from which one can see that they quickly dwell at their

respective final values 3.7812V and -602.494V.

Fig. 16 and 17 show the id* and id, and iq* and iq. They

also dwell quickly around their respective steady-state

values.

Figure 11. Inverter current into the grid.

Figure 12. Load currents

The steady-state values from Figs. 15, 16 and 17

are 16.9645Adi , and 33.089Aqi ,

3.7812Vgdv and 602.494Vgqv . Then one can

compute real and reactive power generated by the

inverter and flowing into the grid through PCC point as

20.00kWgd d gq qP v i v i

10.096kVArgq d gd qQ v i v i

They are almost the same as 20kW and -10kVAr, the

settings for the inverter. This shows that the overall

circuit works effectively.

Figure 13. Source currents.

Figure 14. Fundamental component and harmonics of phase a current

into the grid.

International Journal of Electrical Energy, Vol.1, No.1, March 2013

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Figure 15. Reference voltages gdv and gqv.

Figure 16. *

di and di currents.

Figure 17. *

qi and qi currents.

Fig. 18 shows the three-phase voltage at the inverter

terminal and their fundamental components. The PCC

phase-a voltage and the fundamental component of the

phase-a voltage at the inverter terminal are shown in

Fig.19. From these two figures, one can see that before

the closure of the circuit breaker, the fundamental

component of the inverter voltage traces that of PCC

voltage very quickly. Once errors calculated by (14)

through (16) are less than 5 (a pre-set value), the breaker

is closed. Then the inverter terminal voltage experiences

a short-time mild disturbance, which lasts less than two

cycles. Finally, the inverter terminal voltages dwell at

their steady-state values.

Fig. 20 and 21 show the harmonic components of the

voltage at inverter terminal and PCC point. One can see

that the harmonic components of voltage generated by the

inverter have been filtered out by the resonant inverter

effectively, leaving negligible components at PCC, as can

be seen from Fig. 21.

Figure 18. Inverter terminal voltages and their extracted fundamentals by windowed-sinc filter.

Figure 19. Fundamentals of inverter terminal voltages and voltage at PCC.

Figure 20. Fundamental component and harmonics of phase a voltage at inverter terminal and PCC.

Figure 21. Harmonics of phase a voltage at inverter terminal and PCC.

The control and filter algorithms are implemented in

Simulink. Instead of using z-function or s-function, this

paper adopted a C-language mimicking Simulink

environment based Matlab-script approach to implement

control algorithm. Such an approach is closer to DSP or

microcontroller implementation[11].

IV. CONCLUSION

This paper presents a detailed study on an inverter with

series-connected resonant filter. The relationship between

the THD and power injection from the inverter into the

grid shows that in order to keep the THD under limit,

there is a requirement on the minimum power injection

International Journal of Electrical Energy, Vol.1, No.1, March 2013

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Page 6: Design of Grid Connected Three-phase Inverter … of Grid Connected Three-phase Inverter with Series Resonant Filter and Reduced Control over Synchronization and Real and Reactive

into the grid for a chosen inductance and capacitance in

the filter. This paper also presents a technique to

synchronize the inverter with the power grid at the point

of common coupling. This synchronization algorithm is

part of the control of the real power and reactive power

injection into the grid. The computed numerical results

justify the validity of the proposed topology and its power

control algorithm.

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Daming Zhang received his bachelor's and

master's degrees from Huazhong University of

Science and Technological University in 1993

and 1996, respectively. He worked in Guoce Corporation, China from 1996 to 1997. From

1999 to 2003, he was with Institute of High Performance Computing, China. He was with

Nanyang Technological University from May

of 2003 to January 2012 as an assistant professor. He is now with the School of EE&T, University of New

South Wales as a lecturer, Sydney, Australia. His research interests include filter design for power system application,

characterization of magnetic materials, application of Jiles-

Atherton model to study harmonics, conducted EMI, inrush current, transient and non-linear phenomena in power electronics

converters and design of kilohertz to MHz transformers and inductors for switch-mode power converters. He has also interest

in partial discharge in condition monitoring and numerical

computation of electric field and magnetic fields in power engineering.

Eliathamby Ambikairajah received his BSc(Eng) degree from the University of Sri

Lanka and received his PhD degree in Signal

Processing from Keele University, UK. He

was appointed as Head of Electronic

Engineering and later Dean of Engineering at the Athlone Institute of Technology in the

Republic of Ireland. He was an invited Research Fellow with British Telecom

Laboratories (BTL), Martlesham Heath, England, for 10 years

(1989-1999). He joined the University of New South Wales, Australia in 1999 where he is currently the Head of School of

Electrical Engineering and Telecommunications. Professor Ambikairajah received the Vice-Chancellor’s Award for Teaching

Excellence in April 2004 for his innovative use of educational

technology.

International Journal of Electrical Energy, Vol.1, No.1, March 2013

17©2013 Engineering and Technology Publishing