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International Journal of Modern Engineering Research (IJMER)
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645

Total Harmonic Distortion Alleviation by using Shunt Active Filter
Y.Praveen Kumar Reddy, B. Kumuda, U. Shantha Kumar
Asst. Professor, Dept. of EEE, CBIT, Proddatur,Andra Pradesh, India
Asst. Professor Dept. of EEE, RYMEC, Bellary, Karnataka, India
Asst. Professor, Dept. of EEE, RYMEC, Bellary, Karnataka, India

ABSTRACT: This paper presents a new topology for multilevel Current source converter. The new converter uses
parallel connections of full-bridge cells. Also by Adding or removing the full-bridge cells, modularized circuit layout and
packaging is possible, where the number of output current levels can also be easily adjusted. Using adequate levels, the
multilevel current converter generates approximately sinusoidal output current with very low harmonic distortion. Based on
this converter a shunt active filter has been modeled. The simulation results of the lacking shunt active filter and through
shunt active filter in controlled rectifier shows that the THD alleviation by means of shunt active filter.

Key words: Multilevel Converter, Shunt Active Power Filter, Power Quality.
I.

INTRODUCTION

Recently multilevel power conversion technology has been a very rapidly growing area of power electronics with
good potential for further developments. The most attractive applications of this technology are in the medium to highvoltage range[1] Multilevel converters work more like amplitude modulation rather than pulse modulation, and as a result:
β€’ Each device in a multilevel converter has a much lower dv/dt The outputs of the converter have almost perfect
currents with very good voltage waveforms because the undesirable harmonics can be removed easily,
β€’ The bridges of each converter work at a very low switching frequency and low speed semiconductors can be used and
β€’ Switching losses are very low [2].
The general function of the multilevel converter is to synthesize a desired output voltage from sev- eral levels of DC
voltages as inputs. The DC volt- age sources are available from batteries, capacitors, or fuel cells. There are three types of
multilevel con-verters:
β€’ Diode-Clamped Multilevel Converter
β€’ Flying-Capacitor Multilevel Converter
β€’ Cascaded-Converters with Separated DC Sources
The first practical multilevel topology is the diode-clamped multilevel converter topology and first in-troduced by
Nabae in 1980 [3]. The converter uses capacitors in series to divide the DC bus voltage into a set of voltage levels. To
produce N levels of the phase voltage, an N βˆ’level diode-clamp converter needs N-1 capacitors on the DC bus. The flying
capacitor multilevel converter proposed by Meynard and Foch in 1992 [4], [5]. The converter uses a ladder structure of the DC
side capacitors where the volt-age on each capacitor differs from that of the next capacitor. To generate N βˆ’level staircase
output volt-age, N βˆ’ 1 capacitors in the DC bus are needed.Each phase-leg has an identical structure. The size of the voltage
increment between two capacitors de-termines the size of the voltage levels in the out-put waveform The last structure
introduced in the paper is a multilevel converter, which uses cascade converters with separate DC sources and first used for
plasma stabilization [6], it was then extended for three-phase applications [7]. The multilevel converter using cascadedconverter with separate DC sources synthesizes a desired voltage from several independent sources of DC voltage. A primary
advantage of this topology is that it provides the flexibility to increase the number of levels without introducing
complexity into the power stage. Also, this topology requires the same number of primary switches as the diode-clamped
topology, but does not require the clamping diode. However, this configuration uses multiple dedicated DC-busses and often a
complicated and expensive line transformer, which makes this a rather expensive solution. In addition, bidirectional
operation is somewhat difficult (although not impossible) to achieve [8]. Modularized circuit layout and packaging is
possible because each level has the same structure, and there are no extra clamping diodes or voltage balancing capacitor. The
number of output voltage levels can be adjusted by adding or removing the full-bridge cells The converters that were focused
upon were volt-age source converters, with multilevel voltage wave-forms. These converters divide the total input voltage among
a number switches, and allow a reduction of the voltage harmonics. As mentioned, these are the most commonly used and bestunderstood multilevel converters. The most multilevel converters discussed in the literature are multilevel voltage source con
verters [9]. However, in many current applications, such as shunt active filters, active power line conditioners, VAR
compensations etc., we need to use multilevel current converters. This paper presents a new multilevel current converter. Then
the proposed multilevel current source converter is the core of a shunt active filter, which is obtained based on this converter. The
proposed new multilevel current converter consists of a set of par-allel single-phase full-bridge converter units. The AC current
output of each levels full-bridge converter is connected in parallel such that the synthesized current waveform is the sum of
the converter outputs. In other words, for high current applications many switches can be placed in parallel, with their current
summed by inductors.

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II.

International Journal of Modern Engineering Research (IJMER)
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645

THE PROPOSED MULTILEVEL CURRENT CONVERTER

II.1.The Proposed Topology
The full-bridge topology is used to synthesize a three-level square-wave output current waveform. The full-bridge
configuration of the single-phase current source converter is shown in Fig1.
In as single-phase full-bridge configuration, four switches are needed. In full-bridge configuration, by

Fig.1. A multi level current converter
Turning the switches S1 and S4 on and S2 and S3 off a current of Idc1 is available at output io1, while reversing the ing the
operation we get current of idc1. To generate zero level of a full-bridge converter, the switches S1and S3 are turned on while S2
and S4 are turned off or vice versa. The typical output waveform of full bridge of single-phase multilevel shown in Fig.1 is
shown in Fig. 2

Fig.2.Typical output wave form of three level configuration
The three possible levels with respect to above discussion are shown in Table 1. Note that S1 and S2 should not be open at the
same time, nor should S3 and S4. Otherwise, an open circuit would exist across the DC current source.
Table 1: output current with corresponding conditions
MODES CONDUCTING
OUTPUT
SWITCHES
CURRNT
1
S1,S4
+Idc1
2
S2,S3
-Idc1
3
S1,S3 or S2,S4
0
Fig.3 shows equivalent circuits of the proposed topology at different modes.

Fig.3.The Equivalent Circuits of the Proposed Topology at Different Modes
From Fig. 3, the instantaneous switches voltages of each module are given in Table2
Table 2: Instantaneous switches voltages
Mode
Vs1
Vs2
Vs3
Vs4
1

0

Vo(t)

Vo(t)

0

2

-Vo(t)

0

0

-Vo(t)

3

0

Vo(t)

0

-Vo(t)

Using parallel connections of many converters like the one shown in Fig. 1, we can synthesize multi-level current
converter. The general function of this multilevel current source converter is to synthesize a desired current from several
independent sources of DC currents. Fig. 3 shows a single-phase struc-ture of a parallel converter with a separate DC cur-rent
source. By different combinations of the four switches, S1βˆ’S4, each full-bridge converter can gener-ate three different current
outputs, +Idc1, βˆ’Idc1 and zero current. The AC outputs of each of the different level of full-bridge converters are connected in
par-allel such that the synthesized current waveform is the sum of the converter outputs. An output phase current waveform
is obtained by summing the output currents of the converter bridges:
𝐼 𝑂𝑁 𝑑 = 𝑖 π‘œ1 𝑑 + 𝑖 π‘œ2 𝑑 + β‹― + 𝑖 π‘œπ‘› 𝑑
(1)
Where N is the number of parallel bridges [10].
In the following we propose a new method for determining the levels of different DC current sources, which are used in the
proposed multilevel converter.
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2945 | Page
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International Journal of Modern Engineering Research (IJMER)
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645

Fig.3. Single phase parllel multilevel current source converter
II.2. DETERMINING THE LEVELS
If all DC current sources in Fig. 3 are equal to Idc the converter is then known as symmetric multilevel current source
converter. With having a number of full-bridge converter units, this technique results in an output current of the converter
that is almost sinusoidal.
The maximum output current of the N paralleled multilevel current source converter is
𝐼 𝑀𝐴𝑋 = 𝑁 βˆ— 𝐼 𝑑𝑐
(2)
In this topology; the number of overall output current(S) is given by:
𝑆 = 1 + 2𝑁
(3)
For example, a 13-level multilevel current source converter using the technique can be implemented as shown in Fig. 4. In Fig.
4, io1 to io6 are DC current supplies, which are from either regulated inductors or separated DC sources.

Fig.4 The 13 level converter output

III.

THE SHUNT ACTIVE FILTER BASED ON MULTILEVEL CURRENT SOURCE
CONVER-TER

III. 1.SHUNT ACTIVE FILTER PRINCIPLE
In recent years, the usage of modern electronic equipment has been increasing rapidly. These elect-ronic equipments
impose nonlinear loads to the AC main that draw reactive and harmonic current in ad-dition to active current. In order to
overcome these problems, different kinds of active power fil-ters, based on force-commutated devices, have been developed.
Particularly, shunt active power filters, using different control strategies, have been widely investigated. These filters operate
as current sources, connected in parallel with the nonlinear load generat-ing the current and the current harmonic components
required by the load. However, shunt active filters present the disadvantages that are difficult to imple-ment in large scale
where the control is also compli-cated. To reduce the drawbacks, the proposed solu-tion in this paper is to use a multilevel
current source converter. A shunt active filter consists of a controllable voltage or current source. This topology is shown in
fig.5 it consisting of DC link capacitor C, power electronic switch and inductor Lf.

Fig.5 configuration of voltage source converter based on shunt active filter
III.2. SUGGESTED SHUNT ACTIVE FILTER
Fig.6 shows the schematic of the suggested shunt active power filter consisting of the new multilevel current source
inverter with a control unit, to solve the power quality problems. The operation of the shunt current source multilevel
inverters is based on the injection of current harmonic, i SH , which is in phase with the load current, iLoad, thus eliminating the
harmonic current of the line(supply) current iLine. Now, suppose that the load current can be written as the sum of the
fundamental and harmonic current as in equation (4)
𝑖 πΏπ‘œπ‘Žπ‘‘ = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,𝐹𝑒𝑛𝑑 + 𝑖 πΏπ‘œπ‘Žπ‘‘ ,π»π‘Žπ‘Ÿπ‘šπ‘œπ‘›π‘–π‘π‘ 
(4)
Then the injected current by shunt inverter should be:
𝑖 𝑆𝐻 = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,π»π‘Žπ‘Ÿπ‘šπ‘œπ‘›π‘–π‘π‘ 
(5)
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2946 | Page
International Journal of Modern Engineering Research (IJMER)
www.ijmer.com
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645
With resulting the line current
𝑖 𝐿𝑖𝑛𝑒 = 𝑖 πΏπ‘œπ‘Žπ‘‘ βˆ’ 𝑖 𝑆𝐻
(6)
𝑖 𝐿𝑖𝑛𝑒 = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,πΉπ‘œπ‘’π‘›π‘‘
(7)
As it is seen, the equation (7) only contains the fundamental component of the load current and thus free from the harmonics.

Fig.6. Suggested Shunt Active filter configuration

IV.

WITHOUT SHUNT ACTIVE FILTER

The industrial loads usually have complex nonlinear dynamics. In connecting nonlinearities to a power network, they induce
some undesirable distortions to the sinusoidal signal of the network. For showing this effect, a three phase controlled rectifier is
used as a nonlinear load connected to grid Fig.7 shows the circuit of a three-phase controlled rectifier. The input phase voltages can
be written as:
𝑣 π‘Ž = 𝑣 π‘š 𝑠𝑖𝑛𝑀 𝑖 𝑑
(8)
𝑣 𝑏 = 𝑣 π‘š sin 𝑀 𝑖 𝑑 βˆ’ 2πœ‹ 3
(9)
𝑣 𝑐 = 𝑣 π‘š sin 𝑀 𝑖 𝑑 + 2πœ‹ 3
(10)

Fig.7. Three Phase Controlled Rectifier as a Nonlinear Load
If the load is assumed a pure resistance, the output current Peak is:
𝐼 𝑀𝐴𝑋

= √3𝑉 π‘š

𝑅𝐿

(11)

In this study, the parameters of the system are as 𝑉 π‘š = 110√2 𝑉, 𝑀 𝑖 = 100πœ‹ π‘Žπ‘›π‘‘ 𝑅 𝐿 = 40ohms Fig.8 shows waveforms of
input line voltages, load current and line currents. As the Fig.8 shows, nonlinear loads may pollute power lines seriously
with their high levels harmonic current and reduction in power factor. Fig.9 depicts the Fast Fourier Transform of ac utility
line current Harmonics up to the 20th have been considered. The THD of the input current of the rectifier also the ac utility
line current is 103.87%.

Fig.8. The Outputs of Controlled Rectifier

Fig.9. FFT analysis of the line current of Controlled Rectifier
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International Journal of Modern Engineering Research (IJMER)
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645

V.

WITH SHUNT ACTIVE FILTER

The ability of shunt active filters to suppress these problems has attracted a great deal of attention to these systems.
This paper proposed a new struc-ture for shunt active filter based on multilevel cur-rent source converter. For showing the
capability of the proposed shunt active filter, a 13 level multilevel current source converter as shown in Fig.10. Fig.11.
Shows a single phase structure of the

Fig.10. 13 level current converter
Multilevel converter. The converter consists of seven full-bridges with all current sources are equal to Idc. Fig. 12
shows the load, line and shunt active power filter output currents. The shunt active power filter with multilevel current
converter is able to successfully compensates reactive power and mitigate current harmonics distortions with excellent
transient performance.

Fig.11. Single-Phase 13-Level Multilevel Current Converter Used in the Shunt Active Filter System
Fig.13. depicts the Fast Fourier Transform of ac utility line current Harmonics with shunt active filter up to the 20th
have been considered. The THD of the input current of the rectifier also the ac utility line current is 12.66%.

VI.

CONCLUSION

In this paper, a new topology for multilevel current source converters has been presented. The most important feature of the
system is being convenient for expanding and increasing the Number of output levels. The proposed strategies generate a
current with minimum error with respect to the sinusoidal reference. Therefore, it generates very low harmonic distortion.
Load currents

Shunt active filter currents

Line currents

Fig.12. Load, Shunt Active Filter and Line Output Currents
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International Journal of Modern Engineering Research (IJMER)
Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949
ISSN: 2249-6645

Fig.12. FFT analysis of the line current iA, at ac utility connected through shunt active filter

REFERENCES
[1]
[2]
[3]
[4]
[5]
[6]
[7]
[8]
[9]
[10]

Nikola Celanovic, β€œSpace Vector Modulation and Control of Multilevel Converters," Ph.D. Thesis, Blacksburg, Virginia, Sep.
2000.
Giri Venkataramanan, and Ashish Bendre,” Reciprocity-Transposition-Based Sinusoidal Pulse width Modulation for DiodeClamped Multilevel Converters," IEEE Transaction on Industrial Electronics, Vol. 49, No. 5, pp. 1035-1047, Oct. 2002.
Nabae, I. Takahashi and H. Akagi, β€œA New Neutral-Point Clamped PWM Inverter," IEEE Transactions on Industry Applications,
Vol. IA-17, No.5, pp. 518-523, September=October 1981.
T. Meynard and H. Foch, β€œMulti-Level Conversion: High Voltage Choppers and Voltage Source Inverters," IEEE PESC92, pp.
397403, 1992.
T. Meynard and H. Foch”Imbricated Cells Multi-Level Voltage Source Inverters for High Voltage Applications," European Power
Electronics Journal, Vol. 3, No. 2, pp. 99106, June 1993.
M. Marchesoni, M. Mazzucchelli and S. Tenconi, β€œA Non Conventional Power Converter for Plasma Stabilization," IEEE
Transactions on Power Electronics, Vol. 5, No. 2, April 1990.
F. Z. Peng, J. S. Lai, J. McKeever and J. Van Coevering, β€œA Multilevel Voltage-Source Inverter with Separate DC Sources for
Static Var Generation," IEEE-IAS Conference Record, pp. 2541-2548, 1995.
J. Rodriguez, L. Moran, A, Gonzales and C.Silva,β€œHigh Voltage Converter with Regeneration Capability," IEEE-PESC Conference
Proceedings, Vol. 2, pp. 1077-1082, 1999.
Geoffrey R. Walker B.E. (Hons), β€œModulation of Multilevel Converters," Ph.D. Thesis, Queensland, Nov. 1999.
Ebrahim Babaei, Seyed Hossein Hosseini and Mahrdad Tarafdar Haque,β€œA Novel Approach to Multilevel Current Source
Converters," Proceedings of the 2005 Electrical Engineering/Electronics, Telecommunications and Information Technology
International Conference (ECTI-CON 2005), Vol. I, pp. 177-180, 12-13 May 2005, Pattaya, Choburi, Thailand.

Y Praveen Kumar Reddy received the B.E (Electrical and Electronics Engineering) degree from the
Jawaharlal Nehru Technological University in 2006 and M.Tech (Power Electronics) in 2008 from the same
university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Chaitanya
Bharathi Institute of Technology . Proddatur. Field of interest includes Renewable Energy Sources, Power
Electrical & Drives,Control Systems.
B. Kumuda received the B.E (Electrical and Electronics Engineering) degree from the Visveswaraiah
Technological University,Belgaum in 2008 and M.Tech (Digital Electronics) in 2011 from the same
university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Rao Bahadur Y
Mahabaleshwarappa Engineering College ,Bellary. Field of interest includes Renewable Energy Sources,
Power Electrical & Drives,Control Systems.
U. Shantha Kumar received the B.Tech (Electrical and Electronics Engineering) degree from the
Jawaharlal Nehru Technological University in 2009 and M.Tech (Power Electronics) in 2012 from the same
university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Rao Bahadur Y
Mahabaleshwarappa Engineering College,Bellary. Field of interest includes Power Systems, Power
Electronics & Drives, Renewable Energy Sources.

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Total Harmonic Distortion Alleviation by using Shunt Active Filter

  • 1. www.ijmer.com International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 Total Harmonic Distortion Alleviation by using Shunt Active Filter Y.Praveen Kumar Reddy, B. Kumuda, U. Shantha Kumar Asst. Professor, Dept. of EEE, CBIT, Proddatur,Andra Pradesh, India Asst. Professor Dept. of EEE, RYMEC, Bellary, Karnataka, India Asst. Professor, Dept. of EEE, RYMEC, Bellary, Karnataka, India ABSTRACT: This paper presents a new topology for multilevel Current source converter. The new converter uses parallel connections of full-bridge cells. Also by Adding or removing the full-bridge cells, modularized circuit layout and packaging is possible, where the number of output current levels can also be easily adjusted. Using adequate levels, the multilevel current converter generates approximately sinusoidal output current with very low harmonic distortion. Based on this converter a shunt active filter has been modeled. The simulation results of the lacking shunt active filter and through shunt active filter in controlled rectifier shows that the THD alleviation by means of shunt active filter. Key words: Multilevel Converter, Shunt Active Power Filter, Power Quality. I. INTRODUCTION Recently multilevel power conversion technology has been a very rapidly growing area of power electronics with good potential for further developments. The most attractive applications of this technology are in the medium to highvoltage range[1] Multilevel converters work more like amplitude modulation rather than pulse modulation, and as a result: β€’ Each device in a multilevel converter has a much lower dv/dt The outputs of the converter have almost perfect currents with very good voltage waveforms because the undesirable harmonics can be removed easily, β€’ The bridges of each converter work at a very low switching frequency and low speed semiconductors can be used and β€’ Switching losses are very low [2]. The general function of the multilevel converter is to synthesize a desired output voltage from sev- eral levels of DC voltages as inputs. The DC volt- age sources are available from batteries, capacitors, or fuel cells. There are three types of multilevel con-verters: β€’ Diode-Clamped Multilevel Converter β€’ Flying-Capacitor Multilevel Converter β€’ Cascaded-Converters with Separated DC Sources The first practical multilevel topology is the diode-clamped multilevel converter topology and first in-troduced by Nabae in 1980 [3]. The converter uses capacitors in series to divide the DC bus voltage into a set of voltage levels. To produce N levels of the phase voltage, an N βˆ’level diode-clamp converter needs N-1 capacitors on the DC bus. The flying capacitor multilevel converter proposed by Meynard and Foch in 1992 [4], [5]. The converter uses a ladder structure of the DC side capacitors where the volt-age on each capacitor differs from that of the next capacitor. To generate N βˆ’level staircase output volt-age, N βˆ’ 1 capacitors in the DC bus are needed.Each phase-leg has an identical structure. The size of the voltage increment between two capacitors de-termines the size of the voltage levels in the out-put waveform The last structure introduced in the paper is a multilevel converter, which uses cascade converters with separate DC sources and first used for plasma stabilization [6], it was then extended for three-phase applications [7]. The multilevel converter using cascadedconverter with separate DC sources synthesizes a desired voltage from several independent sources of DC voltage. A primary advantage of this topology is that it provides the flexibility to increase the number of levels without introducing complexity into the power stage. Also, this topology requires the same number of primary switches as the diode-clamped topology, but does not require the clamping diode. However, this configuration uses multiple dedicated DC-busses and often a complicated and expensive line transformer, which makes this a rather expensive solution. In addition, bidirectional operation is somewhat difficult (although not impossible) to achieve [8]. Modularized circuit layout and packaging is possible because each level has the same structure, and there are no extra clamping diodes or voltage balancing capacitor. The number of output voltage levels can be adjusted by adding or removing the full-bridge cells The converters that were focused upon were volt-age source converters, with multilevel voltage wave-forms. These converters divide the total input voltage among a number switches, and allow a reduction of the voltage harmonics. As mentioned, these are the most commonly used and bestunderstood multilevel converters. The most multilevel converters discussed in the literature are multilevel voltage source con verters [9]. However, in many current applications, such as shunt active filters, active power line conditioners, VAR compensations etc., we need to use multilevel current converters. This paper presents a new multilevel current converter. Then the proposed multilevel current source converter is the core of a shunt active filter, which is obtained based on this converter. The proposed new multilevel current converter consists of a set of par-allel single-phase full-bridge converter units. The AC current output of each levels full-bridge converter is connected in parallel such that the synthesized current waveform is the sum of the converter outputs. In other words, for high current applications many switches can be placed in parallel, with their current summed by inductors. www.ijmer.com 2944 | Page
  • 2. www.ijmer.com II. International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 THE PROPOSED MULTILEVEL CURRENT CONVERTER II.1.The Proposed Topology The full-bridge topology is used to synthesize a three-level square-wave output current waveform. The full-bridge configuration of the single-phase current source converter is shown in Fig1. In as single-phase full-bridge configuration, four switches are needed. In full-bridge configuration, by Fig.1. A multi level current converter Turning the switches S1 and S4 on and S2 and S3 off a current of Idc1 is available at output io1, while reversing the ing the operation we get current of idc1. To generate zero level of a full-bridge converter, the switches S1and S3 are turned on while S2 and S4 are turned off or vice versa. The typical output waveform of full bridge of single-phase multilevel shown in Fig.1 is shown in Fig. 2 Fig.2.Typical output wave form of three level configuration The three possible levels with respect to above discussion are shown in Table 1. Note that S1 and S2 should not be open at the same time, nor should S3 and S4. Otherwise, an open circuit would exist across the DC current source. Table 1: output current with corresponding conditions MODES CONDUCTING OUTPUT SWITCHES CURRNT 1 S1,S4 +Idc1 2 S2,S3 -Idc1 3 S1,S3 or S2,S4 0 Fig.3 shows equivalent circuits of the proposed topology at different modes. Fig.3.The Equivalent Circuits of the Proposed Topology at Different Modes From Fig. 3, the instantaneous switches voltages of each module are given in Table2 Table 2: Instantaneous switches voltages Mode Vs1 Vs2 Vs3 Vs4 1 0 Vo(t) Vo(t) 0 2 -Vo(t) 0 0 -Vo(t) 3 0 Vo(t) 0 -Vo(t) Using parallel connections of many converters like the one shown in Fig. 1, we can synthesize multi-level current converter. The general function of this multilevel current source converter is to synthesize a desired current from several independent sources of DC currents. Fig. 3 shows a single-phase struc-ture of a parallel converter with a separate DC cur-rent source. By different combinations of the four switches, S1βˆ’S4, each full-bridge converter can gener-ate three different current outputs, +Idc1, βˆ’Idc1 and zero current. The AC outputs of each of the different level of full-bridge converters are connected in par-allel such that the synthesized current waveform is the sum of the converter outputs. An output phase current waveform is obtained by summing the output currents of the converter bridges: 𝐼 𝑂𝑁 𝑑 = 𝑖 π‘œ1 𝑑 + 𝑖 π‘œ2 𝑑 + β‹― + 𝑖 π‘œπ‘› 𝑑 (1) Where N is the number of parallel bridges [10]. In the following we propose a new method for determining the levels of different DC current sources, which are used in the proposed multilevel converter. www.ijmer.com 2945 | Page
  • 3. www.ijmer.com International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 Fig.3. Single phase parllel multilevel current source converter II.2. DETERMINING THE LEVELS If all DC current sources in Fig. 3 are equal to Idc the converter is then known as symmetric multilevel current source converter. With having a number of full-bridge converter units, this technique results in an output current of the converter that is almost sinusoidal. The maximum output current of the N paralleled multilevel current source converter is 𝐼 𝑀𝐴𝑋 = 𝑁 βˆ— 𝐼 𝑑𝑐 (2) In this topology; the number of overall output current(S) is given by: 𝑆 = 1 + 2𝑁 (3) For example, a 13-level multilevel current source converter using the technique can be implemented as shown in Fig. 4. In Fig. 4, io1 to io6 are DC current supplies, which are from either regulated inductors or separated DC sources. Fig.4 The 13 level converter output III. THE SHUNT ACTIVE FILTER BASED ON MULTILEVEL CURRENT SOURCE CONVER-TER III. 1.SHUNT ACTIVE FILTER PRINCIPLE In recent years, the usage of modern electronic equipment has been increasing rapidly. These elect-ronic equipments impose nonlinear loads to the AC main that draw reactive and harmonic current in ad-dition to active current. In order to overcome these problems, different kinds of active power fil-ters, based on force-commutated devices, have been developed. Particularly, shunt active power filters, using different control strategies, have been widely investigated. These filters operate as current sources, connected in parallel with the nonlinear load generat-ing the current and the current harmonic components required by the load. However, shunt active filters present the disadvantages that are difficult to imple-ment in large scale where the control is also compli-cated. To reduce the drawbacks, the proposed solu-tion in this paper is to use a multilevel current source converter. A shunt active filter consists of a controllable voltage or current source. This topology is shown in fig.5 it consisting of DC link capacitor C, power electronic switch and inductor Lf. Fig.5 configuration of voltage source converter based on shunt active filter III.2. SUGGESTED SHUNT ACTIVE FILTER Fig.6 shows the schematic of the suggested shunt active power filter consisting of the new multilevel current source inverter with a control unit, to solve the power quality problems. The operation of the shunt current source multilevel inverters is based on the injection of current harmonic, i SH , which is in phase with the load current, iLoad, thus eliminating the harmonic current of the line(supply) current iLine. Now, suppose that the load current can be written as the sum of the fundamental and harmonic current as in equation (4) 𝑖 πΏπ‘œπ‘Žπ‘‘ = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,𝐹𝑒𝑛𝑑 + 𝑖 πΏπ‘œπ‘Žπ‘‘ ,π»π‘Žπ‘Ÿπ‘šπ‘œπ‘›π‘–π‘π‘  (4) Then the injected current by shunt inverter should be: 𝑖 𝑆𝐻 = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,π»π‘Žπ‘Ÿπ‘šπ‘œπ‘›π‘–π‘π‘  (5) www.ijmer.com 2946 | Page
  • 4. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 With resulting the line current 𝑖 𝐿𝑖𝑛𝑒 = 𝑖 πΏπ‘œπ‘Žπ‘‘ βˆ’ 𝑖 𝑆𝐻 (6) 𝑖 𝐿𝑖𝑛𝑒 = 𝑖 πΏπ‘œπ‘Žπ‘‘ ,πΉπ‘œπ‘’π‘›π‘‘ (7) As it is seen, the equation (7) only contains the fundamental component of the load current and thus free from the harmonics. Fig.6. Suggested Shunt Active filter configuration IV. WITHOUT SHUNT ACTIVE FILTER The industrial loads usually have complex nonlinear dynamics. In connecting nonlinearities to a power network, they induce some undesirable distortions to the sinusoidal signal of the network. For showing this effect, a three phase controlled rectifier is used as a nonlinear load connected to grid Fig.7 shows the circuit of a three-phase controlled rectifier. The input phase voltages can be written as: 𝑣 π‘Ž = 𝑣 π‘š 𝑠𝑖𝑛𝑀 𝑖 𝑑 (8) 𝑣 𝑏 = 𝑣 π‘š sin 𝑀 𝑖 𝑑 βˆ’ 2πœ‹ 3 (9) 𝑣 𝑐 = 𝑣 π‘š sin 𝑀 𝑖 𝑑 + 2πœ‹ 3 (10) Fig.7. Three Phase Controlled Rectifier as a Nonlinear Load If the load is assumed a pure resistance, the output current Peak is: 𝐼 𝑀𝐴𝑋 = √3𝑉 π‘š 𝑅𝐿 (11) In this study, the parameters of the system are as 𝑉 π‘š = 110√2 𝑉, 𝑀 𝑖 = 100πœ‹ π‘Žπ‘›π‘‘ 𝑅 𝐿 = 40ohms Fig.8 shows waveforms of input line voltages, load current and line currents. As the Fig.8 shows, nonlinear loads may pollute power lines seriously with their high levels harmonic current and reduction in power factor. Fig.9 depicts the Fast Fourier Transform of ac utility line current Harmonics up to the 20th have been considered. The THD of the input current of the rectifier also the ac utility line current is 103.87%. Fig.8. The Outputs of Controlled Rectifier Fig.9. FFT analysis of the line current of Controlled Rectifier www.ijmer.com 2947 | Page
  • 5. www.ijmer.com International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 V. WITH SHUNT ACTIVE FILTER The ability of shunt active filters to suppress these problems has attracted a great deal of attention to these systems. This paper proposed a new struc-ture for shunt active filter based on multilevel cur-rent source converter. For showing the capability of the proposed shunt active filter, a 13 level multilevel current source converter as shown in Fig.10. Fig.11. Shows a single phase structure of the Fig.10. 13 level current converter Multilevel converter. The converter consists of seven full-bridges with all current sources are equal to Idc. Fig. 12 shows the load, line and shunt active power filter output currents. The shunt active power filter with multilevel current converter is able to successfully compensates reactive power and mitigate current harmonics distortions with excellent transient performance. Fig.11. Single-Phase 13-Level Multilevel Current Converter Used in the Shunt Active Filter System Fig.13. depicts the Fast Fourier Transform of ac utility line current Harmonics with shunt active filter up to the 20th have been considered. The THD of the input current of the rectifier also the ac utility line current is 12.66%. VI. CONCLUSION In this paper, a new topology for multilevel current source converters has been presented. The most important feature of the system is being convenient for expanding and increasing the Number of output levels. The proposed strategies generate a current with minimum error with respect to the sinusoidal reference. Therefore, it generates very low harmonic distortion. Load currents Shunt active filter currents Line currents Fig.12. Load, Shunt Active Filter and Line Output Currents www.ijmer.com 2948 | Page
  • 6. www.ijmer.com International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 5, Sep - Oct. 2013 pp-2944-2949 ISSN: 2249-6645 Fig.12. FFT analysis of the line current iA, at ac utility connected through shunt active filter REFERENCES [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] Nikola Celanovic, β€œSpace Vector Modulation and Control of Multilevel Converters," Ph.D. Thesis, Blacksburg, Virginia, Sep. 2000. Giri Venkataramanan, and Ashish Bendre,” Reciprocity-Transposition-Based Sinusoidal Pulse width Modulation for DiodeClamped Multilevel Converters," IEEE Transaction on Industrial Electronics, Vol. 49, No. 5, pp. 1035-1047, Oct. 2002. Nabae, I. Takahashi and H. Akagi, β€œA New Neutral-Point Clamped PWM Inverter," IEEE Transactions on Industry Applications, Vol. IA-17, No.5, pp. 518-523, September=October 1981. T. Meynard and H. Foch, β€œMulti-Level Conversion: High Voltage Choppers and Voltage Source Inverters," IEEE PESC92, pp. 397403, 1992. T. Meynard and H. Foch”Imbricated Cells Multi-Level Voltage Source Inverters for High Voltage Applications," European Power Electronics Journal, Vol. 3, No. 2, pp. 99106, June 1993. M. Marchesoni, M. Mazzucchelli and S. Tenconi, β€œA Non Conventional Power Converter for Plasma Stabilization," IEEE Transactions on Power Electronics, Vol. 5, No. 2, April 1990. F. Z. Peng, J. S. Lai, J. McKeever and J. Van Coevering, β€œA Multilevel Voltage-Source Inverter with Separate DC Sources for Static Var Generation," IEEE-IAS Conference Record, pp. 2541-2548, 1995. J. Rodriguez, L. Moran, A, Gonzales and C.Silva,β€œHigh Voltage Converter with Regeneration Capability," IEEE-PESC Conference Proceedings, Vol. 2, pp. 1077-1082, 1999. Geoffrey R. Walker B.E. (Hons), β€œModulation of Multilevel Converters," Ph.D. Thesis, Queensland, Nov. 1999. Ebrahim Babaei, Seyed Hossein Hosseini and Mahrdad Tarafdar Haque,β€œA Novel Approach to Multilevel Current Source Converters," Proceedings of the 2005 Electrical Engineering/Electronics, Telecommunications and Information Technology International Conference (ECTI-CON 2005), Vol. I, pp. 177-180, 12-13 May 2005, Pattaya, Choburi, Thailand. Y Praveen Kumar Reddy received the B.E (Electrical and Electronics Engineering) degree from the Jawaharlal Nehru Technological University in 2006 and M.Tech (Power Electronics) in 2008 from the same university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Chaitanya Bharathi Institute of Technology . Proddatur. Field of interest includes Renewable Energy Sources, Power Electrical & Drives,Control Systems. B. Kumuda received the B.E (Electrical and Electronics Engineering) degree from the Visveswaraiah Technological University,Belgaum in 2008 and M.Tech (Digital Electronics) in 2011 from the same university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Rao Bahadur Y Mahabaleshwarappa Engineering College ,Bellary. Field of interest includes Renewable Energy Sources, Power Electrical & Drives,Control Systems. U. Shantha Kumar received the B.Tech (Electrical and Electronics Engineering) degree from the Jawaharlal Nehru Technological University in 2009 and M.Tech (Power Electronics) in 2012 from the same university. Currently an Asst. Professor of the Dept. Electrical and Electronics Engineering, Rao Bahadur Y Mahabaleshwarappa Engineering College,Bellary. Field of interest includes Power Systems, Power Electronics & Drives, Renewable Energy Sources. www.ijmer.com 2949 | Page