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ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012



 Neuro-Fuzzy Five-level Cascaded Multilevel Inverter
              for Active Power Filter
                    G.Nageswara Rao1, Dr.K.Chandra Sekhar2, and Dr.P.Sangameswara Raju2
                               1
                                   Vijaya Institute of Technology for Women, Vijayawada, India
                                                  Email: gnrgudipudi@gmail.com
                                        2
                                          RVR & JC College of Engineering, Guntur, India
                                                     Email: cskoritala@gmail.com
                                                  3
                                                    S.V.University, Tirupathi, India
                                                    Email: raju_2000@yahoo.com

Abstract—This paper presents an investigation of five-Level            series active power filter, is employed for voltage correction
Cascaded H-bridge(CHB) inverter as Active Power Filter in             and is connected in line with the NLL [1-7]. Power quality
Power System (PS) for compensation of reactive power and              (PQ) is the key to successful delivery of quality product and
harmonics. The advantages of CHB inverter are low harmonic            operation of an industry. The term PQ means to maintain
distortion, reduced number of switches and suppression of
                                                                      purely sinusoidal current waveform in phase with a purely
switching losses. The Active Power Filter helps to improve
the power factor and eliminate the Total Harmonics Distortion         sinusoidal voltage waveform. The deteriorating quality of
(THD) drawn from a Non-Liner Diode Rectifier Load (NLDRL).            electric power is mainly because of current and voltage
The D-Q reference frame theory is used to generate the                harmonics due to wide spread application of static power
reference compensating currents for Active Power Filter               converters, zero and negative sequence components
while Neuro-Fuzzy controller(NFC) is used for capacitor dc            originated by the use of single phase and unbalanced loads,
voltage regulation. A CHB Inverter is considered for shunt            reactive power, voltage sag, voltage swell, flicker, voltage
compensation of a 11 kV distribution system. Finally a level          interruption etc. The cascade multilevel inverter based active
shifted PWM (LSPWM) technique adopted to investigate the              power filter is suitable for power line conditioning in the power
performance of CHB Inverter. The results are obtained through
                                                                      distribution network[8]. A hierarchical neuro-fuzzy current
Mat lab / Simulink .
                                                                      control scheme for a shunt active power filter improve the
Index Terms— Active power filter(APF), Five-level cascade             performance[9].
inverter, level shifted pulse width modulation(LSPWM),                    The power conversion strategy called multilevel
neuro-fuzzy controller(NFC),total harmonic distortion(THD),           inversion decreases the total harmonic distortion (THD)
harmonics.                                                            by obtaining the output voltage in steps and bringing the
                                                                      output closer to a sine wave [10]. Producing an approximate
                      I. INTRODUCTION                                 sinusoidal voltage from multiple levels of dc voltages,
    The widespread increase of non-linear loads nowadays,             normally obtained from capacitor voltage sources is the
significant amounts of harmonic currents are being injected           common objective of multilevel inverters [11]. A multi-pulse
into power systems. Harmonic currents flow through the power          inverter like 6-pulse or 12-pulse inverter achieves harmonic
system impedance, causing voltage distortion at the harmonic          as well as reactive power (VAR) compensation through
currents’ frequencies. The distorted voltage waveform causes          numerous voltage-source inverters interconnected in a zigzag
harmonic currents to be drawn by other loads connected at             manner by means of transformers [12]. Flexibe ac transmission
the point of common coupling (PCC). The existence of current          systems, renewable energy sources, uninterruptible power
and voltage harmonics in power systems increases losses in            supplies and active power filters are some power electronics
the lines, decreases the power factor and can cause timing            applications in which multilevel inverters are important [13].
errors in sensitive electronic equipments. The use of grid            Multi-level inverters (MLI) have emerged as a successful
connected power electronic converters to improve power                and realistic solution for power increase and harmonics
quality in power distribution systems represents the best             reduction of AC waveform [14].
solution, in terms of performance and stability, for the                  This paper presents various issues in design of Neuro-
elimination of harmonic distortion, power factor correction,          Fuzzy controller and level shifted carrier (LSCPWM)
balancing of loads, and voltage regulation.                           technique are used to obtain switching logic for Active power
    The most common example of this type of equipment is              filter. The performance of these controllers is demonstrated
the active power filter (APF) which has two main                      with linear resistive-inductive (R-L) loads through simulation
configurations: the shunt connected active power filter is            results using Power System toolboxes (PST) of Simulink /
placed in parallel with a non-linear load (NLL) and controlled        MATLAB.
to cancel the current harmonics created by it; its dual, the
  G.Nageswara Rao: Tel. No. +91-9247876900, Email Address:
  gnrgudipudi@gmail.com .

© 2012 ACEEE                                                     49
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ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012


 II. DESIGN OF MULTILEVEL INVERTER BASED ACTIVE POWER                 The controller input is an error signal obtained from the refer-
                         FILTER                                       ence voltage and the rms terminal voltage measured. Such
                                                                      error is processed by a neuro-fuzzy controller; the output is
A. Active power filter
                                                                      the angle δ, which is provided to the PWM signal generator
    The increased severity of harmonic pollution in power             as shown in Fig.2. It is important to note that in this case, of
networks has attracted the attention of power electronics             indirectly controlled converter, there is active and reactive
and power system engineers to develop dynamic and                     power exchange with the network simultaneously. The neuro-
adjustable solutions to the power quality problems. Such              fuzzy controller processes the error signal and generates the
equipments, generally known as active filters [15], are also          required angle to drive the error to zero, i.e. the load rms
called active power line conditioners. To effectively                 voltage is brought back to the reference voltage.
compensate the line current harmonics, the active filter
controller should be designed to meet the following three             C. Neuro-Fuzzy Controller
goals:                                                                     Neuro fuzzy system gives the switching angles and
1. extract harmonic currents and inject compensating                  frequency value. By using this value the harmonic contents
current;                                                              present in the system are eliminated. The overall process
2. maintain a constant dc capacitor voltage;                          takes place in proposed method is shown in Fig.4. Feed back
3. avoid generating or absorbing reactive power with                  controller used here is to calculate voltage error values in the
fundamental frequency components.                                     system. This voltage error values is given as the input to
    The shunt APF shown in Fig.1 has the structure of a               neuro fuzzy system. In the feedback controller, the voltage
multilevel voltage source inverter connected to the line by           values are calculated from the voltage waveform for different
an inductance Lf rated at about 5% of the filter power. The dc        time values. From the reference waveform voltage values at
link storage component is a capacitor, usually of larger value        different time values are taken as reference voltage value.
than in a standard power inverter [8].                                Then for different time values, the voltage values are taken
                                                                      from the harmonics waveform and compared with the
                                                                      reference waveform. The voltage error values are calculated
                                                                      using the equation given below.




               Figure 1. Shunt active power filter

B. Control for dc link voltage                                                          Figure 3. Proposed method

    The aim of the control scheme is to maintain constant                                                                         (1)
voltage magnitude at the point where a sensitive load under                            Verror  Vref  Vh
system disturbances is connected. The control system only             where Vref is the voltage value of the system without
measures the rms voltage at the load point, i.e., no reactive
                                                                      harmonics.
power measurements are required. The VSC switching
                                                                         After calculating the voltage error values, next step is to
strategy is based on a sinusoidal PWM technique which
                                                                      generate training dataset for training neuro fuzzy system.
offers simplicity and good response. Since custom power is
                                                                      Generating training dataset is one of the most important
a relatively low-power application, PWM methods offer a
                                                                      processes because based on the training dataset only the
more flexible option than the fundamental frequency
                                                                      neuro fuzzy system will be trained.
switching methods favored in FACTS applications. Apart from
                                                                           The training dataset generated for training neuro fuzzy
this, high switching frequencies can be used to improve on
the efficiency of the converter, without incurring significant        system consists of n input variables and s  1 output
switching losses.                                                     variables. Here, stands for number of voltage values taken
                                                                      for generating dataset, is the total number of dataset
                                                                      generated, is the switching angle and stands for number of
                                                                      switching angles. The dataset generated for our proposed
                                                                      method is shown below.

  Figure.2 Neuro-fuzzy control for reactive power compensation



© 2012 ACEEE                                                     50
DOI: 01.IJEPE.03.01. 93_5
ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012


    V t 11 V t 12 ...... V t 1 n        11  12 ......  1 n                        fuzzy system and h is the harmonic order.  .
                                                               
    V t 21 V t 22 ...... V t 2 n        21  22 ......  2 n                        By substituting equation 5 in 1 we get the output dc voltage.
D  .                                 .                                              The harmonics content eliminated or not is calculated using
                                                                          (2)
    .                                 .                                              the below condition.
    V      V      ...... V tr 1             r 2 ......  r 1 
     tr 1 tr 2                         r1                      

By using the above dataset, neuro fuzzy system is trained.                                            Vref (t )  V (t ); harmonics eliminated
The neuro fuzzy operation is explained briefly in the below                                           
                                                                                              H eli  
sections.                                                                                             Vref (t )  V (t ); harmonics present
The steps for training the neural network are
                                                                                                      
Step 1: Initialize the input weight of each neuron.                                      D. Cascaded H-Bridge Multilevel Inverter
Step 2: Apply a training dataset to the network.
       Here Y1 , Y2 , … Yn are the input to the network and

         Z1 , Z 2 , … Z s 1 are the output of the network.
                                 n
                          Z1   W2 r1Z ( r )                                 (3)
                               r 1    1
                                 n
                          Z 2   W2 r 2 Z ( r )                                              Figure.4 Circuit of the single cascaded H-Bridge Inverter
                                r 1      2
                                                                              (4)           Fig.4 shows the circuit model of a single CHB inverter
                         n                                                    (5)        configuration. By using single H-Bridge we can get 3 voltage
               Z s 1   W2 r ( s 1) Z s 1 ( r )                                      levels. The number of output voltage levels of CHB is given
where,                  r 1                                                             by 2n+1 and voltage step of each level is given by Vdc/2n,
                                                                                         where n is number of H-bridges connected in cascaded. The
                                                                                         switching table is given in Table.I.
                                                                              (6)
                                          1                                                        TABLE I. SWITCHING TABLE OF SINGLE CHB INVERTER
               Z (r )                      n
                          1  exp(  w11r   Y ( k ))
                                           k 1
Eqn 12, 13, 14 & 15 represents the activation function
performed in the output and input layer respectively.
Step 3: Adjust the weights of all neurons.
Step 4: For each set of voltage values, select the
switching angle and frequency.
Step 5: Select the best switching angle and frequency.
    After completion of training, neuro fuzzy is used for
practical application. After completion of training neuro fuzzy
system the next step is to eliminate the harmonic contents in
the system. First voltage error values are calculated using
the equation 3. By giving voltage error values as input to the
neuro fuzzy system, it gives corresponding frequency and
switching angles as output. By applying this frequency and                                    Figure.5. Block diagram of 5-level CHB inverter model
switching angle values to the system the harmonic contents
                                                                                         The switching mechanism for 5-level CHB inverter is shown
present in the system are eliminated. The frequency and
                                                                                         in table-II.
switching angle are substituted in the equation given below.
                                                                                                 Table II. Switching table for 5-level CHB Inverter
                                                                              (7)
                V (t )  Vh . sin(h.2. . f f .t )
where, f f     is the frequency obtained from neuro fuzzy system.


                        4Vdc S                           (8)
                  V h         cos( h j )
                         h j 1
where,    j     is the switching angles obtained from neuro

© 2012 ACEEE                                                                        51
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ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012


                 III. DESIGN OF SINGLE H-BRIDGE CELL                                              Here ‘n’ depends on the switching frequency.
                                                                                                 After considering the DC-Link voltage variations, switching
A. Device Current
                                                                                                 losses of the IGBT can be written as follows.
    The IGBT and DIODE currents can be obtained from the
load current by multiplying with the corresponding duty                                                                Psw ( IGBT )  f sw                            (17)
cycles. Duty cycle, d = ½(1+Kmsinωt), Where, m = modulation                                      So, the sum of conduction and switching losses is the total
index K = +1 for IGBT, -1 for Diode. For a load current given                                    losses given by
by
                                                                                                                  PT ( IGBT )  Pon ( IGBT )  Psw ( IGBT )           (18)
                  I ph               2 ISin (t   )                                (9)
                                                                                                 C. Diode Loss Calculation
Then the device current can be written as follows.
                                                                                                    The DIODE switching losses consist of its reverse
                              2                                                                  recovery losses; the turn-on losses are negligible.
      i d e v ic e                I S in (  t   ) x (1  k m sin  t )          (10)
                           2                                                                                                                  2
The average value of the device current over a cycle is                                                          E rec    a  bI  cI                                (19)
calculated as
                                                                                                                               Psw ( DIODE )  f sw                   (20)
                   
             1                 2                                                                 So, the sum of conduction and switching losses gives the
   iavg 
            2
                             2
                                   ISin(t   ) x(1  km sin t ) dwt               (11)        total DIODE looses.
                       

                                                                                                                  P ( DIODE )
                                                                                                                   T
                                                                                                                                   Pon ( DIODE )  Psw ( DIODE )     (21)
B. IGBT Loss Calculation
                                                                                                 The total loss per one switch (IGBT+DIODE) is the sum of
    IGBT loss can be calculated by the sum of switching loss                                     one IGBT and DIODE loss.
and conduction loss. The conduction loss can be calculated
by,                                                                                                               PT
                                                                                                                          PT ( IGBT )  Psw ( DIODE )                (22)
                                                                 2
            ( Pon ( IGBT )  Vceo  I avg ( igbt )  I rms ( igbt )   ceo          (12)        D. Thermal Calculations
                                                                                                     The junction temperatures of the IGBT and DIODE are
                                              1 m                                              calculated based on the device power losses and thermal
              I avg ( igbt )           2I
                                              2  g cos  
                                                           
                                                                                    (13)         resistances. The thermal resistance equivalent circuit for a
                                                                                                 module is shown in fig-7. In this design the thermal
                                             1 m                                               calculations are started with heat sink temperature as the
             I rms ( igbt )           2I
                                              g  3 cos  
                                                           
                                                                                    (14)         reference temperature. So, the case temperature from the
                                                                                                 model can be written as follows.
Values of Vceo and rceo at any junction temperature can be
obtained from the output characteristics (Ic vs. Vce) of the                                              Tc    PT Rth ( c  h )  Th                                (23)
IGBT as shown in Fig .6.                                                                         Here Rth(c-h) = Thermal resistance between case and heat sink
                                                                                                          PT  TotalPowerLoss ( IGBT  DIODE )                        (24)
                                                                                                 IGBT junction temperature is the sum of the case temperature
                                                                                                 and temperature raise due to the power losses in the IGBT.

                                                                                                                     PT ( IGBT ) Rth ( j  c ) IGBT  Tc
                                                                                                                T j ( IGBT )                              (25)
                                                                                                 The DIODE junction temperature is the sum of the case
                                                                                                 temperature and temperature raise due to the power losses in
                                                                                                 the DIODE.
                       Figure.6. IGBT output characteristics                                                      T j ( DIODE )    PT ( DIODE ) Rth ( DIODE )  Tc   (26)
The switching losses are the sum of all turn-on and turn-off
                                                                                                 The above calculations are done based on the average power
energies at the switching events
                                                                                                 losses computed over a cycle. So, the corresponding thermal
                  E sw  E on  E off  a  bI  cI                                 (15)         calculation gives the average junction temperature. In order
Here VDC is the actual DC-Link voltage and Vnom is the DC-                                       to make the calculated values close to the actual values,
Link Voltage at which Esw is given. Switching losses are                                         transient temperature values are to be added to the average
calculated by summing up the switching energies.                                                 junction temperatures.
Here ‘n’ depends on the switching frequency.
                                         1
                              Psw 
                                        T0
                                                n
                                                     E sw (i )                      (16)

© 2012 ACEEE                                                                                52
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ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012


E. Level Shifted Carrier PWM (LSCPWM)Technique




                                                                                    Fig. 9 phase opposite disposition (POD)

                                                                         IV. MATLAB/SIMULINK MODELING AND SIMULATION RESULTS
                                                                            Fig.10. shows the Matab / Simulink power circuit model
            Figure-7 Level shifted carrier PWM (IPD)                    of APF. It consists of five blocks named as source block, non
Fig.7. shows the Level shifted carrier pulse width modulation.          linear load block, control block, APF block and measurements
An m-level Cascaded H-bridge inverter using level shifted               block. The system parameters for simulation study are source
modulation requires (m–1) triangular carriers, all having the           voltage of 11kv, 50Hz AC supply, DC bus capacitance 1550ìF,
same frequency and amplitude. For PID modulation, the                   Inverter series inductance 10mH, Source resistance of 0.1ohm
multilevel converter with multilevel requires (m1) triangular           and inductance of 0.9mH. Load resistance and inductance
carriers with same amplitude and frequency.                             are chosen as 30mH and 60ohms respectively.
The frequency modulation index ‘mf’ which can be
expressed as
                      mf     f cr / fm                    (27)
where fm is modulating frequency and fcr are carrier waves
frequency.
The amplitude modulation index ‘ma’ is defined by
           ma  Vm / Vcr ( m 1) for 0  ma  1            (28)
Where Vm is the peak value of the modulating wave and Vcr
is the peak value of the each carrier wave [1]. The amplitude
modulation index, ma is 1 and the frequency modulation in-
dex, mf is 6. The triggering circuit is designed based on the                    Fig-10 Matlab/Simulink power circuit model of APF
three phase sinusoidal modulation waves Va, Vb, and Vc. Three           Level shifted carrier PWM technique results
of the sine wave sources have been obtained with same am-                  Fig. 11. shows the phase-A voltage of five level output of
plitude and frequency but displaced 120° out of the phase               level shifted carrier PWM inverter.
with each others. For carriers wave sources block param-
eters, the time values of each carrier waves are set to [0 1/600
1/300] while the outputs values are set according to the dis-
position of carrier waves. After comparing, the output sig-
nals of comparator are transmitted to the IGBTs. Figures 8, 9
and 11shows the waveforms based on three schemes of level
shifted multilevel modulations: (a) in phase disposition (IPD)                       Figure.11. five level LSCPWM output
fig.7, where all carriers are in phase; (b) alternative phase
                                                                        Fig.12. shows the three phase source voltages, three phase
opposite disposition (APOD) Fig.8, where all carriers are al-
                                                                        source currents and load currents respectively without APF.
ternatively in opposite disposition; and (c) phase opposite
                                                                        It is clear that without APF load current and source currents
disposition (POD) fig.9, where all carriers above zero refer-
                                                                        are same.
ence are in phase but in opposition with those below the zero
reference [1]. Out of IPD, APOD and POD; we found that,
IPD give better harmonic performance.




                                                                         Figure.12. Source voltage, current and load current without APF
                                                                        Fig.13 shows the three phase source voltages, three phase
                                                                        source currents and load currents respectively with APF. It is
    Figure. 8. Alternative phase opposite disposition (APOD)            clear that with APF even though load current is non sinusoi-
                                                                        dal source currents are sinusoidal.

© 2012 ACEEE                                                       53
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ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012


                                                                       results are presented.

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Power Filter with five-level CHB Multilevel inverter is                active filters”, IEEE Trans. Ind. Appl., vol. 37, no. 1, pp. 81–89,
investigated for LSCPWM. The source voltage, load voltage,             Jan./Feb. 2001.
source current, load current, power factor and THD simulation
results under non-linear loads are investigated. Finally
Matlab/Simulink based model is developed and simulation
© 2012 ACEEE                                                      54
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Neuro-Fuzzy Five-level Cascaded Multilevel Inverter for Active Power Filter

  • 1. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 Neuro-Fuzzy Five-level Cascaded Multilevel Inverter for Active Power Filter G.Nageswara Rao1, Dr.K.Chandra Sekhar2, and Dr.P.Sangameswara Raju2 1 Vijaya Institute of Technology for Women, Vijayawada, India Email: gnrgudipudi@gmail.com 2 RVR & JC College of Engineering, Guntur, India Email: cskoritala@gmail.com 3 S.V.University, Tirupathi, India Email: raju_2000@yahoo.com Abstract—This paper presents an investigation of five-Level series active power filter, is employed for voltage correction Cascaded H-bridge(CHB) inverter as Active Power Filter in and is connected in line with the NLL [1-7]. Power quality Power System (PS) for compensation of reactive power and (PQ) is the key to successful delivery of quality product and harmonics. The advantages of CHB inverter are low harmonic operation of an industry. The term PQ means to maintain distortion, reduced number of switches and suppression of purely sinusoidal current waveform in phase with a purely switching losses. The Active Power Filter helps to improve the power factor and eliminate the Total Harmonics Distortion sinusoidal voltage waveform. The deteriorating quality of (THD) drawn from a Non-Liner Diode Rectifier Load (NLDRL). electric power is mainly because of current and voltage The D-Q reference frame theory is used to generate the harmonics due to wide spread application of static power reference compensating currents for Active Power Filter converters, zero and negative sequence components while Neuro-Fuzzy controller(NFC) is used for capacitor dc originated by the use of single phase and unbalanced loads, voltage regulation. A CHB Inverter is considered for shunt reactive power, voltage sag, voltage swell, flicker, voltage compensation of a 11 kV distribution system. Finally a level interruption etc. The cascade multilevel inverter based active shifted PWM (LSPWM) technique adopted to investigate the power filter is suitable for power line conditioning in the power performance of CHB Inverter. The results are obtained through distribution network[8]. A hierarchical neuro-fuzzy current Mat lab / Simulink . control scheme for a shunt active power filter improve the Index Terms— Active power filter(APF), Five-level cascade performance[9]. inverter, level shifted pulse width modulation(LSPWM), The power conversion strategy called multilevel neuro-fuzzy controller(NFC),total harmonic distortion(THD), inversion decreases the total harmonic distortion (THD) harmonics. by obtaining the output voltage in steps and bringing the output closer to a sine wave [10]. Producing an approximate I. INTRODUCTION sinusoidal voltage from multiple levels of dc voltages, The widespread increase of non-linear loads nowadays, normally obtained from capacitor voltage sources is the significant amounts of harmonic currents are being injected common objective of multilevel inverters [11]. A multi-pulse into power systems. Harmonic currents flow through the power inverter like 6-pulse or 12-pulse inverter achieves harmonic system impedance, causing voltage distortion at the harmonic as well as reactive power (VAR) compensation through currents’ frequencies. The distorted voltage waveform causes numerous voltage-source inverters interconnected in a zigzag harmonic currents to be drawn by other loads connected at manner by means of transformers [12]. Flexibe ac transmission the point of common coupling (PCC). The existence of current systems, renewable energy sources, uninterruptible power and voltage harmonics in power systems increases losses in supplies and active power filters are some power electronics the lines, decreases the power factor and can cause timing applications in which multilevel inverters are important [13]. errors in sensitive electronic equipments. The use of grid Multi-level inverters (MLI) have emerged as a successful connected power electronic converters to improve power and realistic solution for power increase and harmonics quality in power distribution systems represents the best reduction of AC waveform [14]. solution, in terms of performance and stability, for the This paper presents various issues in design of Neuro- elimination of harmonic distortion, power factor correction, Fuzzy controller and level shifted carrier (LSCPWM) balancing of loads, and voltage regulation. technique are used to obtain switching logic for Active power The most common example of this type of equipment is filter. The performance of these controllers is demonstrated the active power filter (APF) which has two main with linear resistive-inductive (R-L) loads through simulation configurations: the shunt connected active power filter is results using Power System toolboxes (PST) of Simulink / placed in parallel with a non-linear load (NLL) and controlled MATLAB. to cancel the current harmonics created by it; its dual, the G.Nageswara Rao: Tel. No. +91-9247876900, Email Address: gnrgudipudi@gmail.com . © 2012 ACEEE 49 DOI: 01.IJEPE.03.01. 93_5
  • 2. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 II. DESIGN OF MULTILEVEL INVERTER BASED ACTIVE POWER The controller input is an error signal obtained from the refer- FILTER ence voltage and the rms terminal voltage measured. Such error is processed by a neuro-fuzzy controller; the output is A. Active power filter the angle δ, which is provided to the PWM signal generator The increased severity of harmonic pollution in power as shown in Fig.2. It is important to note that in this case, of networks has attracted the attention of power electronics indirectly controlled converter, there is active and reactive and power system engineers to develop dynamic and power exchange with the network simultaneously. The neuro- adjustable solutions to the power quality problems. Such fuzzy controller processes the error signal and generates the equipments, generally known as active filters [15], are also required angle to drive the error to zero, i.e. the load rms called active power line conditioners. To effectively voltage is brought back to the reference voltage. compensate the line current harmonics, the active filter controller should be designed to meet the following three C. Neuro-Fuzzy Controller goals: Neuro fuzzy system gives the switching angles and 1. extract harmonic currents and inject compensating frequency value. By using this value the harmonic contents current; present in the system are eliminated. The overall process 2. maintain a constant dc capacitor voltage; takes place in proposed method is shown in Fig.4. Feed back 3. avoid generating or absorbing reactive power with controller used here is to calculate voltage error values in the fundamental frequency components. system. This voltage error values is given as the input to The shunt APF shown in Fig.1 has the structure of a neuro fuzzy system. In the feedback controller, the voltage multilevel voltage source inverter connected to the line by values are calculated from the voltage waveform for different an inductance Lf rated at about 5% of the filter power. The dc time values. From the reference waveform voltage values at link storage component is a capacitor, usually of larger value different time values are taken as reference voltage value. than in a standard power inverter [8]. Then for different time values, the voltage values are taken from the harmonics waveform and compared with the reference waveform. The voltage error values are calculated using the equation given below. Figure 1. Shunt active power filter B. Control for dc link voltage Figure 3. Proposed method The aim of the control scheme is to maintain constant (1) voltage magnitude at the point where a sensitive load under Verror  Vref  Vh system disturbances is connected. The control system only where Vref is the voltage value of the system without measures the rms voltage at the load point, i.e., no reactive harmonics. power measurements are required. The VSC switching After calculating the voltage error values, next step is to strategy is based on a sinusoidal PWM technique which generate training dataset for training neuro fuzzy system. offers simplicity and good response. Since custom power is Generating training dataset is one of the most important a relatively low-power application, PWM methods offer a processes because based on the training dataset only the more flexible option than the fundamental frequency neuro fuzzy system will be trained. switching methods favored in FACTS applications. Apart from The training dataset generated for training neuro fuzzy this, high switching frequencies can be used to improve on the efficiency of the converter, without incurring significant system consists of n input variables and s  1 output switching losses. variables. Here, stands for number of voltage values taken for generating dataset, is the total number of dataset generated, is the switching angle and stands for number of switching angles. The dataset generated for our proposed method is shown below. Figure.2 Neuro-fuzzy control for reactive power compensation © 2012 ACEEE 50 DOI: 01.IJEPE.03.01. 93_5
  • 3. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 V t 11 V t 12 ...... V t 1 n    11  12 ......  1 n  fuzzy system and h is the harmonic order. .     V t 21 V t 22 ...... V t 2 n    21  22 ......  2 n  By substituting equation 5 in 1 we get the output dc voltage. D  .  .  The harmonics content eliminated or not is calculated using     (2) .  .  the below condition. V V ...... V tr 1    r 2 ......  r 1   tr 1 tr 2   r1  By using the above dataset, neuro fuzzy system is trained. Vref (t )  V (t ); harmonics eliminated The neuro fuzzy operation is explained briefly in the below  H eli   sections. Vref (t )  V (t ); harmonics present The steps for training the neural network are  Step 1: Initialize the input weight of each neuron. D. Cascaded H-Bridge Multilevel Inverter Step 2: Apply a training dataset to the network. Here Y1 , Y2 , … Yn are the input to the network and Z1 , Z 2 , … Z s 1 are the output of the network. n Z1   W2 r1Z ( r ) (3) r 1 1 n Z 2   W2 r 2 Z ( r ) Figure.4 Circuit of the single cascaded H-Bridge Inverter r 1 2 (4) Fig.4 shows the circuit model of a single CHB inverter n (5) configuration. By using single H-Bridge we can get 3 voltage Z s 1   W2 r ( s 1) Z s 1 ( r ) levels. The number of output voltage levels of CHB is given where, r 1 by 2n+1 and voltage step of each level is given by Vdc/2n, where n is number of H-bridges connected in cascaded. The switching table is given in Table.I. (6) 1 TABLE I. SWITCHING TABLE OF SINGLE CHB INVERTER Z (r )  n 1  exp(  w11r   Y ( k )) k 1 Eqn 12, 13, 14 & 15 represents the activation function performed in the output and input layer respectively. Step 3: Adjust the weights of all neurons. Step 4: For each set of voltage values, select the switching angle and frequency. Step 5: Select the best switching angle and frequency. After completion of training, neuro fuzzy is used for practical application. After completion of training neuro fuzzy system the next step is to eliminate the harmonic contents in the system. First voltage error values are calculated using the equation 3. By giving voltage error values as input to the neuro fuzzy system, it gives corresponding frequency and switching angles as output. By applying this frequency and Figure.5. Block diagram of 5-level CHB inverter model switching angle values to the system the harmonic contents The switching mechanism for 5-level CHB inverter is shown present in the system are eliminated. The frequency and in table-II. switching angle are substituted in the equation given below. Table II. Switching table for 5-level CHB Inverter (7) V (t )  Vh . sin(h.2. . f f .t ) where, f f is the frequency obtained from neuro fuzzy system. 4Vdc S (8) V h  cos( h j ) h j 1 where, j is the switching angles obtained from neuro © 2012 ACEEE 51 DOI: 01.IJEPE.03.01. 93_5
  • 4. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 III. DESIGN OF SINGLE H-BRIDGE CELL Here ‘n’ depends on the switching frequency. After considering the DC-Link voltage variations, switching A. Device Current losses of the IGBT can be written as follows. The IGBT and DIODE currents can be obtained from the load current by multiplying with the corresponding duty Psw ( IGBT )  f sw (17) cycles. Duty cycle, d = ½(1+Kmsinωt), Where, m = modulation So, the sum of conduction and switching losses is the total index K = +1 for IGBT, -1 for Diode. For a load current given losses given by by PT ( IGBT )  Pon ( IGBT )  Psw ( IGBT ) (18) I ph  2 ISin (t   ) (9) C. Diode Loss Calculation Then the device current can be written as follows. The DIODE switching losses consist of its reverse 2 recovery losses; the turn-on losses are negligible. i d e v ic e  I S in (  t   ) x (1  k m sin  t ) (10) 2 2 The average value of the device current over a cycle is E rec  a  bI  cI (19) calculated as Psw ( DIODE )  f sw (20)   1 2 So, the sum of conduction and switching losses gives the iavg  2  2 ISin(t   ) x(1  km sin t ) dwt (11) total DIODE looses.  P ( DIODE ) T  Pon ( DIODE )  Psw ( DIODE ) (21) B. IGBT Loss Calculation The total loss per one switch (IGBT+DIODE) is the sum of IGBT loss can be calculated by the sum of switching loss one IGBT and DIODE loss. and conduction loss. The conduction loss can be calculated by, PT  PT ( IGBT )  Psw ( DIODE ) (22) 2 ( Pon ( IGBT )  Vceo  I avg ( igbt )  I rms ( igbt )   ceo (12) D. Thermal Calculations The junction temperatures of the IGBT and DIODE are  1 m  calculated based on the device power losses and thermal I avg ( igbt )  2I  2  g cos     (13) resistances. The thermal resistance equivalent circuit for a module is shown in fig-7. In this design the thermal 1 m  calculations are started with heat sink temperature as the I rms ( igbt )  2I  g  3 cos     (14) reference temperature. So, the case temperature from the model can be written as follows. Values of Vceo and rceo at any junction temperature can be obtained from the output characteristics (Ic vs. Vce) of the Tc  PT Rth ( c  h )  Th (23) IGBT as shown in Fig .6. Here Rth(c-h) = Thermal resistance between case and heat sink PT  TotalPowerLoss ( IGBT  DIODE ) (24) IGBT junction temperature is the sum of the case temperature and temperature raise due to the power losses in the IGBT.  PT ( IGBT ) Rth ( j  c ) IGBT  Tc T j ( IGBT ) (25) The DIODE junction temperature is the sum of the case temperature and temperature raise due to the power losses in the DIODE. Figure.6. IGBT output characteristics T j ( DIODE )  PT ( DIODE ) Rth ( DIODE )  Tc (26) The switching losses are the sum of all turn-on and turn-off The above calculations are done based on the average power energies at the switching events losses computed over a cycle. So, the corresponding thermal E sw  E on  E off  a  bI  cI (15) calculation gives the average junction temperature. In order Here VDC is the actual DC-Link voltage and Vnom is the DC- to make the calculated values close to the actual values, Link Voltage at which Esw is given. Switching losses are transient temperature values are to be added to the average calculated by summing up the switching energies. junction temperatures. Here ‘n’ depends on the switching frequency. 1 Psw  T0  n E sw (i ) (16) © 2012 ACEEE 52 DOI: 01.IJEPE.03.01. 93_5
  • 5. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 E. Level Shifted Carrier PWM (LSCPWM)Technique Fig. 9 phase opposite disposition (POD) IV. MATLAB/SIMULINK MODELING AND SIMULATION RESULTS Fig.10. shows the Matab / Simulink power circuit model Figure-7 Level shifted carrier PWM (IPD) of APF. It consists of five blocks named as source block, non Fig.7. shows the Level shifted carrier pulse width modulation. linear load block, control block, APF block and measurements An m-level Cascaded H-bridge inverter using level shifted block. The system parameters for simulation study are source modulation requires (m–1) triangular carriers, all having the voltage of 11kv, 50Hz AC supply, DC bus capacitance 1550ìF, same frequency and amplitude. For PID modulation, the Inverter series inductance 10mH, Source resistance of 0.1ohm multilevel converter with multilevel requires (m1) triangular and inductance of 0.9mH. Load resistance and inductance carriers with same amplitude and frequency. are chosen as 30mH and 60ohms respectively. The frequency modulation index ‘mf’ which can be expressed as mf  f cr / fm (27) where fm is modulating frequency and fcr are carrier waves frequency. The amplitude modulation index ‘ma’ is defined by ma  Vm / Vcr ( m 1) for 0  ma  1 (28) Where Vm is the peak value of the modulating wave and Vcr is the peak value of the each carrier wave [1]. The amplitude modulation index, ma is 1 and the frequency modulation in- dex, mf is 6. The triggering circuit is designed based on the Fig-10 Matlab/Simulink power circuit model of APF three phase sinusoidal modulation waves Va, Vb, and Vc. Three Level shifted carrier PWM technique results of the sine wave sources have been obtained with same am- Fig. 11. shows the phase-A voltage of five level output of plitude and frequency but displaced 120° out of the phase level shifted carrier PWM inverter. with each others. For carriers wave sources block param- eters, the time values of each carrier waves are set to [0 1/600 1/300] while the outputs values are set according to the dis- position of carrier waves. After comparing, the output sig- nals of comparator are transmitted to the IGBTs. Figures 8, 9 and 11shows the waveforms based on three schemes of level shifted multilevel modulations: (a) in phase disposition (IPD) Figure.11. five level LSCPWM output fig.7, where all carriers are in phase; (b) alternative phase Fig.12. shows the three phase source voltages, three phase opposite disposition (APOD) Fig.8, where all carriers are al- source currents and load currents respectively without APF. ternatively in opposite disposition; and (c) phase opposite It is clear that without APF load current and source currents disposition (POD) fig.9, where all carriers above zero refer- are same. ence are in phase but in opposition with those below the zero reference [1]. Out of IPD, APOD and POD; we found that, IPD give better harmonic performance. Figure.12. Source voltage, current and load current without APF Fig.13 shows the three phase source voltages, three phase source currents and load currents respectively with APF. It is Figure. 8. Alternative phase opposite disposition (APOD) clear that with APF even though load current is non sinusoi- dal source currents are sinusoidal. © 2012 ACEEE 53 DOI: 01.IJEPE.03.01. 93_5
  • 6. ACEEE Int. J. on Electrical and Power Engineering, Vol. 03, No. 01, Feb 2012 results are presented. REFERENCES [1] A. Ajami and S. H. Hosseini, “Implementation of a Novel Control Strategy for Shunt Active Filter,” ECTI Transactions On Electrical Eng., Electronics, And Communications. Vol.4, No.1, pp. Figure.13. Source voltage, current and load current with APF 40-46, February 2006. Fig.14. shows the DC bus voltage with respect to time. The [2] M. Ghandchi, A. Ajami and M. Moeini, “A Simple and Low DC bus voltage is regulated to 11kv by using Neuro-Fuzzy Cost Control Strategy for Multilevel Shunt Active Filters,” in Proceeding of International Conference on Control, Automation controller. and Systems 2008 in COEX, Seoul, Korea. pp. 14-17, October 2008 . [3] P. Zanchetta, M. Sumner, M. Marinelli and F. Cupertino, “Experimental modeling and control design of shunt active power filters,” Control Engineering Practice, Vol.17, pp. 1126 – 1135, May 2009. [4] M.George, K. P. Basu, “Three-Phase Shunt Active Power Figure.14. DC Bus Vooltage Filter,” American Journal of Applied Sciences, Vol. 5, No. 8,pp. Fig.15 shows the phase-A source voltage and current, even 909-916, 2008.. [5] M.C. Benhabib, S. Saadate, “ New control approach for four- though the load is non linear RL load the source power factor wire active power filter based on the use of synchronous reference is unity. frame”, Electric Power System Research, Vol.73 , pp. 353–362, 2005. [6] C. Yanbo, Z. Fudan, K.W. E. Cheng, “Shunt Active Power Filter – Simulink Simulation and DSP-based International Conference on Power Electronics Systems and Applications, pp. 120-125, 2006. [7] G. Zhoua, B. Wub, D. Xuc, “Direct power control of a Figure.15. Phase-A source voltage and current multilevel inverter based active power filter”, Electric Power System Fig.16. shows the harmonic spectrum of Phase –A Source Research, Vol.77 , pp. 284–294, 2007. current without APF. The THD of source current without [8] Karuppanan and Kamalakanth mahapatra, “PI,PID and fuzzy logic controlled cascaded voltage source inverter based active power APF is 29.48 %. filter for power line conditioners”, Wseas Transactions on power systems, Issue 4,Vol.6 ,October 2011, pp. 100–109. [9] K.Cagatay Bayindir,M.ugras Cuma,Mehmet Tumay, “Hierarchical neuro-fuzzy current control for a shunt active power filter”, Neural computing and applications ,volume 15, issue 3- 4,pp 223-238, June 2006. [10] S. Jeevananthan, “Evolutionary Computing Based Area Integration PWM Technique for Multilevel Inverters”, Journal of Figure.16 Harmonic spectrum of Phase-A Source current without Electrical Systems, Vol.3, No.2, P.p:61-72, 2007. AP F [11] Eswaran Chandra Sekaran, Ponna Nadar,Anbalagan and Chelliah Fig.17. shows the harmonic spectrum of Phase –A Source Palanisamy, “Analysis and Simulation of a New Shunt Active current with APF. The THD of source current with APF is 7%. Power Filter Using Cascaded Multilevel Inverter “, Journal of Electrical Engineering, Vol. 58, No. 5,pp. 241–249,2007. [12] P.Palanivel, Subhransu Sekher, Dash, “Phase Shifted Carrier Pulse Width Modulation for Three Phase Multilevel Inverter to Minimize THD and Enhance Output Voltage Performance”, Journal of Electrical Systems, Vol.6, No. 2, pp. 1-13, June 2010. [13] A. Hussein. Attia, M. El- Metwally and Osama M. Fahmy, “Harmonic Distortion Effects and Mitigation in Distribution Figure.17. Harmonic spectrum of Phase-A Source current with APF Systems”, Journal of American Science, Vol. 6, No. 10, pp. 173- 183, 2010. CONCLUSION [14] A. F. Zobaa, “Practical Solutions for Harmonics Problems Produced in the Distribution Networks”, Journal of Electrical The Mathematical model for single H-Bridge inverter is Systems, Vol. 2, No.1 pp.13-28, 2006. developed which can be extended to multi H-Bridge. A Active [15] P.Mattavelli,”Aclosed-loop selective harmonic mpensation for Power Filter with five-level CHB Multilevel inverter is active filters”, IEEE Trans. Ind. Appl., vol. 37, no. 1, pp. 81–89, investigated for LSCPWM. The source voltage, load voltage, Jan./Feb. 2001. source current, load current, power factor and THD simulation results under non-linear loads are investigated. Finally Matlab/Simulink based model is developed and simulation © 2012 ACEEE 54 DOI: 01.IJEPE.03.01. 93_5