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Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.180-185
180 | P a g e
Elimination of Harmonics of Induction Furnace by Appling
PQ-Theory for the Control of Hybrid Selective Active Filter
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda
ABSTRACT
This paper describes how to calculate the
different harmonic sequences that should be
filtered with a hybrid selective active filter, for
two control alternatives: load current
measurement or line current measurement. These
results are then generalized for hybrid selective
active filters. Passive parameters are chosen
considering the resonances with the electric
system that appear. Design basis are defined in
order to obtain a minimum cost filter which also
meet the applicable regulations requirements.
In this paper presents a hybrid selective active
filter configuration to mitigate harmonics, which
uses shunt passive and active filters. To obtain the
switching signals for the active filter have used
instantaneous power theory proposed by
H.Akagi. Hybrid selective active filter proposed
scheme has been verified through various
simulations in MATLAB-SIMULINK
environment. Finally, results showing the
potentiality of the selective filter controlled for
the proposed methods are reported.
Keywords - Induction furnace, Hybrid selective
active filter, pq –theory.
I. INTRODUCTION
An Induction furnace is an unbalanced,
nonlinear and time varying load, which can cause
many problems to the power system quality.
Harmonics, inter-harmonics, voltage flicker &
unbalance are the power quality problems which are
introduced to the power system as a result of non-
linear and stochastic behaviour of the furnace
operation [7]. The nonlinear voltage-current
characteristic of the arc can cause harmonic currents
which when circulating by the net can produce
harmonic voltages which can affect to other users [8].
In the last decades, the evolution of two aspects
concerning power systems has created conditions
for a more extended use of active filters. A first
aspect is related to power semiconductor device
development. Converters capable of synthesizing
voltages and currents with an adequate bandwidth
for harmonic current compensation at MVA – level
systems are now available at competitive prices. The
other aspect is the gradual application of regulations
limiting the generation of harmonic currents by the
customers. Active filters are ideally suitable for
filtering localized harmonic currents in a guided
way , this allows to apply the concept ”you dirty, you
clean”. This concept cannot be applied using
conventional passive filters. In the same way, active
filters allows to eliminate some of the problems of
passive filters such as poor tuning due to dispersion
of their characteristic parameters and resonances with
the impedance of the surrounding electrical network
which may appear.
Among the different methods for controlling active
filters, the use of pq-theory (active and imaginary
power) [1], has demonstrated to be specially suitable.
In particular, it has been used for separating the
residual harmonics and thus eliminating (as theory
indicates) or reducing (as it results in practice) the
harmonic distortion. For the control of selective
active filters several works use the SRF method
(Synchronous Reference Frame) [2] [3] [4] [5] [6]
which is definitively a particular case of applying the
pq- method with harmonic voltages as references.
II. INDUCTION FURNACE
One of the most economic ways of
producing steel is made through the use of induction
furnaces. The problem with this kind of furnaces,
from an electrical point of view, is the creation of a
considerable harmonic distortion. The cause of the
distortion is within the induction furnace design and
operation. An induction furnace works melting the
scrap using a medium frequency magnetic field
created by a coil. The coil is fed by the medium
frequency AC current supplied by an inverter which
is fed by a DC current converter connected to the AC
distribution network supply. As the created distortion
is very high and affects the voltage supplied by the
distribution network, it is highly possible that other
loads supplied from the same network will be
affected. In this case, it is necessary to have
corrective actions in order to fulfil the legislation
concerning voltage harmonic distortion. Among these
corrective actions, active filters are one of the most
effective [12].
2.1. SIMULINK MODEL OF THE INDUCTION
FURNACE
All the elements have been modeled using
existing Simulink blocks contained in the
SimPowerSystems block set. The distribution
transformers of the general services and the temper
furnaces consume 1800 kW with a cosφ of 0,85. For
simulation purposes they have been modeled as a
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.
181 | P a g e
lineal load of these characteristics. This is acceptable
as their consumption is only a little portion of the
total power consumed in the plant and they do not
produce any distortion. As there is no induction
furnace electrical model in Simulink, new blocks
have been created for the induction furnaces shown
in fig.2.
Fig.1.Equivalent circuit diagram of induction furnace
Fig. 2.induction furnace without filter
Fig.3. induction furnace load
III. PQ –THEORY
In 1983 Akagi et al.[13],[14] proposed a
new theory for the control of active filters in three-
phase power systems called “Generalized Theory of
The Instantaneous Reactive power in Three phase
Circuits” or “ Theory of Instantaneous Real Power
and Imaginary Power” or “ Theory of Instantaneous
Active power and Reactive power”, or “Theory of the
instantaneous power”, or simply as “p-q Theory”.
Since p-q theory is based on the time domain. It is
valid both for steady-state and transient operation, as
well as for generic voltage and current wave forms,
allowing the control of the active filters in real-time.
Another advantage of this theory is simplicity of
its calculations, since only algebraic operations are
required. The only exception is in the separation of
some power components in their mean and
alternating values. It is possible to exploit the
symmetries of the instantaneous power waveform for
each specific power system, achieving a calculation
delay that can be small as 1/6 and never greater than
1 cycle of the power system frequency. It is also
shown that calculations for reactive power and zero-
sequence compensation do not introduce any delay.
Furthermore, it is possible to associate physical
meaning to the p-q theory power components, which
eases the understanding of the operation of any three-
phase power system , balanced or unbalanced, with
or without harmonics.
3.1. THE P-Q THEORY APPLIED TO HYBRID
SELECTIVE ACTIVE FILTERS.
The p-q theory is one of the several methods that can
be used in the control active filters [13],[15]. It
presents some interesting features, namely:
1-It is inherently a three-phase system theory.
2-It can be applied to any three-phase systems
(balanced or unbalanced, with or without harmonics
in both voltages and currents).
3-It is based in instantaneous values, allowing
excellent dynamic response.
4-It calculations are relatively simple (It only
includes algebraic expressions that can be
implemented using standard processors).
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.
182 | P a g e
5-It allows two control strategies: constant
instantaneous supply power and sinusoidal supply
current.
To control the shunt active filter in such a way as
to present zero impedance for the fundamental and
pure resistance for the harmonics, the reference
output voltage of the shunt active filter is given by
Transformation of the phase voltages ,
, on the load side and source currents sui , svi ,
swi into α-β orthogonal coordinates gives the
following expressions:
(1)
(2)
According to [18], the instantaneous real power p
and the instantaneous imaginary power q can be
defined as:
(3)
The dimension of q is not in watt, volt-ampere, or
var because . and . are defined by
the product of the instantaneous voltage in one phase
and the instantaneous voltage in one phase and the
instantaneous current in the other phase.
The harmonic components Ph and qh are extracted
from p and q by using a high pass filter. A first order
high pass filter, the cutoff frequency of which is 35
hz, is used in the following experiment, filtering
characteristics in the transient states being taken into
account. In the calculation circuit of shi the following
calculations are performed.
(4)
Fig.4..Active power filter controller
Where , A,B,C,and D are the Transfer functions.







 

2
3
2
30
2
1
2
11
3
2
A (5)










LL
LL
VV
VV
B (6)














2
3
2
1
2
3
2
1
01
3
2
C
1






 

LL
LL
VV
VV
(7)







 

2
3
2
30
2
1
2
11
3
2
D (8)
IV. SIMULATION AND PERFORMANCE
INVESTIGATION OF ACTIVE
FILTER
In this section the simulation analysis of Hybrid
selective active filter is described for Induction
Furnace load and the FFT analysis has been carried
out simultaneously.
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.
183 | P a g e
Fig.5.Induction furnace with filter circuit
4.1. SIMULATED RESULTS
Fig 6.shows a set of simulated results of furnace
current, furnace voltage, three phase supply current
with and without using filter. and the THD measured
for all three phase line . The waveform of source
current is close to fundamental sinusoid, showing that
harmonic current is eliminated from the source
current. Therefore, it can be concluded that the
proposed hybrid active filter can compensate
harmonic current.
Fig.6.(a).Furnace current
Fig.6.(b).Furnace voltage
Fig.6.(c)Source current without filter
Fig.6.(d)Source current with filter
Fig.6.(e).THD of supply current Line-1 without
filter
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.
184 | P a g e
Fig.6.(f).THD of supply current Line-2 without filter
Fig.6.(f).THD of supply current Line-3 without filter
Fig.6.(g).THD of supply current Line-1 with filter
Fig.6.(h).THD of supply current Line-2 with filter
Fig.6.(i).THD of supply current Line-3 with filter
THD’s of supply current before and after
filtration
Table 1
Supply current line no. Before
filtration
After
filtration
THD of supply current
Line-1
37.48% 2.02%
THD of supply current
Line-2
34.29% 1.68%
THD of supply current
Line-3
25.43% 1.00%
CONCLUSION
A MATLAB based model of the hybrid active
power filter has been simulated for Induction furnace
load by Appling pq-theory for the control of hybrid
selective active filter. The simulation results show
that the supply current harmonics are compensated
very effectively by using the hybrid selective active
filter.
REFERENCES
[1] H. Akagi, Y. Kanazawa, and A. Nabae,
“Instantaneous reactive power compensator
comprising switching devices without
energy storage components,” IEEE Trans.
Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 3, May-Jun 2013, pp.
185 | P a g e
Ind. Appl., vol. Vol. 20, no. 3, pp. 625–630,
1984.
[2] S. Bhattacharya, P. Cheng, and M. D. Divan,
“Hybrid solutions for improving passive
filter performance in high power
applications,” IEEE Transactions on
Industry Applications, vol. 33, no. 3, pp.
732–747, 1997.
[3] S.Bhattacharya and D. Divan, “Design and
implementation of a hybrid series active
filter system,” IEEE, pp. 189–195, June
1995.
[4] V.S. Ramsden D. Basic and P. Muttik,
“Hybrid filter control system with adaptive
filters for selective elimination of harmonics
and interharmonics,” IEE Proc.-Electr.
Power Appl., vol. 147, no. 3, pp. 295–303,
May 2000.
[5] S.Park J.H.Shung and K.Nam ,“New hybrid
parallel active filter configuration
minimizing active filter size,” IEE Proc.
Electr. Power Appl., vol. 147, no. 2, pp. 93–
98, Mar. 2000.
[6] P. Mattavelli, “A closed-loop selective
harmonic compensation for active filters,”
IEEE Transactions on Industry Applications,
vol. 37, no. 1, pp. 81–89, 2001
[7] M.A.Golkar, M.Tavakoli Bina and S.Meschi
, “ A Novel Method of Electrical Arc
Furnace Modeling for Flicker Study”
[8] Swapnil Arya , Dr. Bhavesh Bhalja ,
“Simulation of Steel Melting Furnace in
MATLAB and its effect on power Quality
problems” , National Conference on Recent
Trends in Engineering & Technology, 13-14
May 2011
[9] M. A. Prieto, M. P. Donsión. "An Improved
Time Domain Arc Furnace Model for
Harmonic Analysis”, IEEE Trans on Power
Delivery, V.19, pp.367-373,2004
[10] Labar Hocine, Dgeghader Yacine, Kelaiaia
Mounia Samira, and Bounaya Kamel”
World Academy of Science, Engineering
and Technology 40 2008
[11] Klaus Timm, Hamburg, basic Principals of
electric furnaces, Edited by E. Plockinger
and O. Etterich, John Wiley and Sons, Ltd,
1985, pp 127- 160
[12] G. Casaravilla, A. Salvia, C. Briozzo and E.
Watanabe ,“Selective active filter applied to
an arc furnace adjusted to harmonic
emission limitations”, Latin America T&D
IEEE Conference, San Pablo - Brasil, 2002
[13] H.Akagi, Y.kanazawa, A. Nabae,
“Generalized theory of the instantaneous
reactive power in three phase circurits,”
IPEC 83-int power electronics conf. Tokyo,
Japan,1983, pp. 1375-1386.
[14] H.Akagi, Y.kanazawa, A. Nabae,
“Instantaneous reactive power compensator
comprising switching devices without
energy storage components”, IEEE Trans
Industry applic, vol.20, may /june 1984.
[15] S-J. Huang and J-C Wu, “ A control
algorithim for three-phase three-wired active
power filters under nonideal mains
voltages,” IEEE Transcations on power
electronics, vol, 14, no,4. Pp. 753-760, july
1999.

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Ag33180185

  • 1. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp.180-185 180 | P a g e Elimination of Harmonics of Induction Furnace by Appling PQ-Theory for the Control of Hybrid Selective Active Filter Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda ABSTRACT This paper describes how to calculate the different harmonic sequences that should be filtered with a hybrid selective active filter, for two control alternatives: load current measurement or line current measurement. These results are then generalized for hybrid selective active filters. Passive parameters are chosen considering the resonances with the electric system that appear. Design basis are defined in order to obtain a minimum cost filter which also meet the applicable regulations requirements. In this paper presents a hybrid selective active filter configuration to mitigate harmonics, which uses shunt passive and active filters. To obtain the switching signals for the active filter have used instantaneous power theory proposed by H.Akagi. Hybrid selective active filter proposed scheme has been verified through various simulations in MATLAB-SIMULINK environment. Finally, results showing the potentiality of the selective filter controlled for the proposed methods are reported. Keywords - Induction furnace, Hybrid selective active filter, pq –theory. I. INTRODUCTION An Induction furnace is an unbalanced, nonlinear and time varying load, which can cause many problems to the power system quality. Harmonics, inter-harmonics, voltage flicker & unbalance are the power quality problems which are introduced to the power system as a result of non- linear and stochastic behaviour of the furnace operation [7]. The nonlinear voltage-current characteristic of the arc can cause harmonic currents which when circulating by the net can produce harmonic voltages which can affect to other users [8]. In the last decades, the evolution of two aspects concerning power systems has created conditions for a more extended use of active filters. A first aspect is related to power semiconductor device development. Converters capable of synthesizing voltages and currents with an adequate bandwidth for harmonic current compensation at MVA – level systems are now available at competitive prices. The other aspect is the gradual application of regulations limiting the generation of harmonic currents by the customers. Active filters are ideally suitable for filtering localized harmonic currents in a guided way , this allows to apply the concept ”you dirty, you clean”. This concept cannot be applied using conventional passive filters. In the same way, active filters allows to eliminate some of the problems of passive filters such as poor tuning due to dispersion of their characteristic parameters and resonances with the impedance of the surrounding electrical network which may appear. Among the different methods for controlling active filters, the use of pq-theory (active and imaginary power) [1], has demonstrated to be specially suitable. In particular, it has been used for separating the residual harmonics and thus eliminating (as theory indicates) or reducing (as it results in practice) the harmonic distortion. For the control of selective active filters several works use the SRF method (Synchronous Reference Frame) [2] [3] [4] [5] [6] which is definitively a particular case of applying the pq- method with harmonic voltages as references. II. INDUCTION FURNACE One of the most economic ways of producing steel is made through the use of induction furnaces. The problem with this kind of furnaces, from an electrical point of view, is the creation of a considerable harmonic distortion. The cause of the distortion is within the induction furnace design and operation. An induction furnace works melting the scrap using a medium frequency magnetic field created by a coil. The coil is fed by the medium frequency AC current supplied by an inverter which is fed by a DC current converter connected to the AC distribution network supply. As the created distortion is very high and affects the voltage supplied by the distribution network, it is highly possible that other loads supplied from the same network will be affected. In this case, it is necessary to have corrective actions in order to fulfil the legislation concerning voltage harmonic distortion. Among these corrective actions, active filters are one of the most effective [12]. 2.1. SIMULINK MODEL OF THE INDUCTION FURNACE All the elements have been modeled using existing Simulink blocks contained in the SimPowerSystems block set. The distribution transformers of the general services and the temper furnaces consume 1800 kW with a cosφ of 0,85. For simulation purposes they have been modeled as a
  • 2. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp. 181 | P a g e lineal load of these characteristics. This is acceptable as their consumption is only a little portion of the total power consumed in the plant and they do not produce any distortion. As there is no induction furnace electrical model in Simulink, new blocks have been created for the induction furnaces shown in fig.2. Fig.1.Equivalent circuit diagram of induction furnace Fig. 2.induction furnace without filter Fig.3. induction furnace load III. PQ –THEORY In 1983 Akagi et al.[13],[14] proposed a new theory for the control of active filters in three- phase power systems called “Generalized Theory of The Instantaneous Reactive power in Three phase Circuits” or “ Theory of Instantaneous Real Power and Imaginary Power” or “ Theory of Instantaneous Active power and Reactive power”, or “Theory of the instantaneous power”, or simply as “p-q Theory”. Since p-q theory is based on the time domain. It is valid both for steady-state and transient operation, as well as for generic voltage and current wave forms, allowing the control of the active filters in real-time. Another advantage of this theory is simplicity of its calculations, since only algebraic operations are required. The only exception is in the separation of some power components in their mean and alternating values. It is possible to exploit the symmetries of the instantaneous power waveform for each specific power system, achieving a calculation delay that can be small as 1/6 and never greater than 1 cycle of the power system frequency. It is also shown that calculations for reactive power and zero- sequence compensation do not introduce any delay. Furthermore, it is possible to associate physical meaning to the p-q theory power components, which eases the understanding of the operation of any three- phase power system , balanced or unbalanced, with or without harmonics. 3.1. THE P-Q THEORY APPLIED TO HYBRID SELECTIVE ACTIVE FILTERS. The p-q theory is one of the several methods that can be used in the control active filters [13],[15]. It presents some interesting features, namely: 1-It is inherently a three-phase system theory. 2-It can be applied to any three-phase systems (balanced or unbalanced, with or without harmonics in both voltages and currents). 3-It is based in instantaneous values, allowing excellent dynamic response. 4-It calculations are relatively simple (It only includes algebraic expressions that can be implemented using standard processors).
  • 3. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp. 182 | P a g e 5-It allows two control strategies: constant instantaneous supply power and sinusoidal supply current. To control the shunt active filter in such a way as to present zero impedance for the fundamental and pure resistance for the harmonics, the reference output voltage of the shunt active filter is given by Transformation of the phase voltages , , on the load side and source currents sui , svi , swi into α-β orthogonal coordinates gives the following expressions: (1) (2) According to [18], the instantaneous real power p and the instantaneous imaginary power q can be defined as: (3) The dimension of q is not in watt, volt-ampere, or var because . and . are defined by the product of the instantaneous voltage in one phase and the instantaneous voltage in one phase and the instantaneous current in the other phase. The harmonic components Ph and qh are extracted from p and q by using a high pass filter. A first order high pass filter, the cutoff frequency of which is 35 hz, is used in the following experiment, filtering characteristics in the transient states being taken into account. In the calculation circuit of shi the following calculations are performed. (4) Fig.4..Active power filter controller Where , A,B,C,and D are the Transfer functions.           2 3 2 30 2 1 2 11 3 2 A (5)           LL LL VV VV B (6)               2 3 2 1 2 3 2 1 01 3 2 C 1          LL LL VV VV (7)           2 3 2 30 2 1 2 11 3 2 D (8) IV. SIMULATION AND PERFORMANCE INVESTIGATION OF ACTIVE FILTER In this section the simulation analysis of Hybrid selective active filter is described for Induction Furnace load and the FFT analysis has been carried out simultaneously.
  • 4. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp. 183 | P a g e Fig.5.Induction furnace with filter circuit 4.1. SIMULATED RESULTS Fig 6.shows a set of simulated results of furnace current, furnace voltage, three phase supply current with and without using filter. and the THD measured for all three phase line . The waveform of source current is close to fundamental sinusoid, showing that harmonic current is eliminated from the source current. Therefore, it can be concluded that the proposed hybrid active filter can compensate harmonic current. Fig.6.(a).Furnace current Fig.6.(b).Furnace voltage Fig.6.(c)Source current without filter Fig.6.(d)Source current with filter Fig.6.(e).THD of supply current Line-1 without filter
  • 5. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp. 184 | P a g e Fig.6.(f).THD of supply current Line-2 without filter Fig.6.(f).THD of supply current Line-3 without filter Fig.6.(g).THD of supply current Line-1 with filter Fig.6.(h).THD of supply current Line-2 with filter Fig.6.(i).THD of supply current Line-3 with filter THD’s of supply current before and after filtration Table 1 Supply current line no. Before filtration After filtration THD of supply current Line-1 37.48% 2.02% THD of supply current Line-2 34.29% 1.68% THD of supply current Line-3 25.43% 1.00% CONCLUSION A MATLAB based model of the hybrid active power filter has been simulated for Induction furnace load by Appling pq-theory for the control of hybrid selective active filter. The simulation results show that the supply current harmonics are compensated very effectively by using the hybrid selective active filter. REFERENCES [1] H. Akagi, Y. Kanazawa, and A. Nabae, “Instantaneous reactive power compensator comprising switching devices without energy storage components,” IEEE Trans.
  • 6. Ramesh Babu P., Ashisa Dash, Smruti Ranjan Panda / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 3, May-Jun 2013, pp. 185 | P a g e Ind. Appl., vol. Vol. 20, no. 3, pp. 625–630, 1984. [2] S. Bhattacharya, P. Cheng, and M. D. Divan, “Hybrid solutions for improving passive filter performance in high power applications,” IEEE Transactions on Industry Applications, vol. 33, no. 3, pp. 732–747, 1997. [3] S.Bhattacharya and D. Divan, “Design and implementation of a hybrid series active filter system,” IEEE, pp. 189–195, June 1995. [4] V.S. Ramsden D. Basic and P. Muttik, “Hybrid filter control system with adaptive filters for selective elimination of harmonics and interharmonics,” IEE Proc.-Electr. Power Appl., vol. 147, no. 3, pp. 295–303, May 2000. [5] S.Park J.H.Shung and K.Nam ,“New hybrid parallel active filter configuration minimizing active filter size,” IEE Proc. Electr. Power Appl., vol. 147, no. 2, pp. 93– 98, Mar. 2000. [6] P. Mattavelli, “A closed-loop selective harmonic compensation for active filters,” IEEE Transactions on Industry Applications, vol. 37, no. 1, pp. 81–89, 2001 [7] M.A.Golkar, M.Tavakoli Bina and S.Meschi , “ A Novel Method of Electrical Arc Furnace Modeling for Flicker Study” [8] Swapnil Arya , Dr. Bhavesh Bhalja , “Simulation of Steel Melting Furnace in MATLAB and its effect on power Quality problems” , National Conference on Recent Trends in Engineering & Technology, 13-14 May 2011 [9] M. A. Prieto, M. P. Donsión. "An Improved Time Domain Arc Furnace Model for Harmonic Analysis”, IEEE Trans on Power Delivery, V.19, pp.367-373,2004 [10] Labar Hocine, Dgeghader Yacine, Kelaiaia Mounia Samira, and Bounaya Kamel” World Academy of Science, Engineering and Technology 40 2008 [11] Klaus Timm, Hamburg, basic Principals of electric furnaces, Edited by E. Plockinger and O. Etterich, John Wiley and Sons, Ltd, 1985, pp 127- 160 [12] G. Casaravilla, A. Salvia, C. Briozzo and E. Watanabe ,“Selective active filter applied to an arc furnace adjusted to harmonic emission limitations”, Latin America T&D IEEE Conference, San Pablo - Brasil, 2002 [13] H.Akagi, Y.kanazawa, A. Nabae, “Generalized theory of the instantaneous reactive power in three phase circurits,” IPEC 83-int power electronics conf. Tokyo, Japan,1983, pp. 1375-1386. [14] H.Akagi, Y.kanazawa, A. Nabae, “Instantaneous reactive power compensator comprising switching devices without energy storage components”, IEEE Trans Industry applic, vol.20, may /june 1984. [15] S-J. Huang and J-C Wu, “ A control algorithim for three-phase three-wired active power filters under nonideal mains voltages,” IEEE Transcations on power electronics, vol, 14, no,4. Pp. 753-760, july 1999.