IRJET- Optimal Control of Multilevel Inverter to Minimize Harmonic Distortion in Photovoltaic Power Generating Array

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 487
OPTIMAL CONTROL OF MULTILEVEL INVERTER TO MINIMIZE
HARMONIC DISTORTION IN PHOTOVOLTAIC POWER
GENERATING ARRAY
SHARAD CHANDRA RAJPOOT1, ISWAR PRASAD PATEL2, DEMAN KOSALE3, PRASHANT SINGH
RAJPOOT4
1Assistant professor (EE) G.E.C. Jagdalpur, Bastar, Chhattisgarh, India,
2M-tech scholar (EE) VEC, Lakhanpur, Ambikapur Chhattisgarh, India
3Assistant professor (EE) VEC, Lakhanpur, Ambikapur Chhattisgarh, India
4Assistant professor (EE) L.C.I.T., Bilaspur, Chhattisgarh, India,
----------------------------------------------------------------------***---------------------------------------------------------------------------
Abstract- In the present scenario power becomes major need for human life. Due to day-to-day increase in population and
lessen of the conventional sources, it becomes necessary that we must depend on non-conventional sources for power
generation. While moving, the vehicles posses some kinetic energy and it is being wasted. Thiskineticenergycanbe utilized to
produce power by using a special arrangement called “POWER HUMP”.TheKineticenergyofmovingvehiclescanbe converted
into mechanical energy of the shaft through rack and pinion mechanism. This shaft is connected to the electric dynamo and it
produces electrical energy proportional to traffic density. This generated power can be regulated by using Zener diode for
continuous supply. All this mechanism can be housed under the dome like speed breaker, which is called hump.
The generated power can be used for general purpose like streetlights, traffic signals.Theelectrical outputcanbeimproved by
arranging these power humps in series this generated power can be amplified and stored by using different electric devices.
The maintenance cost of hump is almost nullified. By adopting this arrangement, we can satisfy the future demands to some
extent.
Index Terms- speed breaker, controller, commutator, power hump, breaking system, OTEC (ocean thermal energy
conversions).
1. INTRODUCTION
1.1 OVERVIEW
Due to the energy shortage, the integration of renewable energy sources to the electricity grid becomes a interesting research
topic nowadays. The number of renewable energy sources and distributed generators is increasingveryfastwhichalsobrings
some threats to the power grid. In order to maintain or even to improve the power supply reliability and quality of the power
system with distributed generation, it is necessary to have some new strategies for the operation and management of the
electricity grid. Modern power electronic technology is an important part in distributed generation and the integration of the
renewable energy to the power grid. It is widely used in the grid based system.
Since the output power of micro-sources (photovoltaic, wind energy etc.) is more or less dependent on the environment
condition such as irradiance and wind, it is necessary to use some specific control strategies or to have some energy storage
system (battery, super-capacitor etc.) in order to compensate forthefluctuations.Onetraditional wayis tousedifferentkindof
converters to integrate the micro sources, energy storage and different types of loads into a common DC bus [2], [3], the basic
structure is shown in Figure 1.
Figure 1. Connection of grid, micro-sources, energy storage systems and load

Some problems with this kind of structure are as follows:
• There are lots of power electronics converters in the system so the harmonics components would be very high, which
increases the cost and size of the harmonics filter.
• If the voltage level is very high, the switching stress of the power electronic device would increase.
• The efficiency would be low due to the power losses in different converters.
To overcome the above shortcomings, a modular power electronics technology named multilevel inverter, which is very
appropriate for the integrating renewable energy source is proposed in [4], [5]. The core idea of the multilevel inverter is to
achieve the desired ac voltage from several levels of dc voltages.
Fig. no. 2 PV array
1.2 Problem identification
Grid connected photovoltaic (PV) powerconversionsystemsaregettingmoreandmoreattentioninthelastdecade, mainlydue
to cost reduction of PV modules and government incentives, which has made this energy source and technology competitive
among other energy sources [13].
2. PV ARRAY MODEL
The output of the PV system is largely dependent on the outside environment conditions. In ordertomakethecorrectanalysis
of the photovoltaic system, a suitable simulation model must be chosen initially.
3. MATHEMATICAL MODEL
PV arrays consist of series and parallel connected PV modules. For each PV module, there are series and parallel connectedPV
cells. The PV cell is usually described by the equivalent circuit shown in Figure 3. It can be seen that one current source anti
parallel with a diode, a shunt and a series resistance are included in the equivalent circuit [14].
The basic equation for the PV cell can be derived by the Kirchhoff’s current law:
I = Isc − Id − Ish (1)
The diode current Id and the shunt branch current Ish can be expressed as






















 1exp0
q
nKT
IRsrV
II
c
d
(2)
sh
sr
sh
R
IRV
I

 (3)
In (1), Isc is defined as the photo current. The value of Isc under reference conditions can be obtained byseeingthedata sheetof
the PV cell. The photocurrent under arbitrary environment conditions can be expressed as:

 )(1 cRcT
r
scRsc TT
R
RII   (4)
Fig. no. 3 PV cell equivalent
Where IscR is the short circuit current at the reference solar radiation RR and the reference cell temperaturewhichareselected
as 1kW/m2 and 25◦C respectively in this thesis. The parameter αT is the temperature coefficientofphotocurrent[14].Andthe
current Io is the dark current which is only the function of cell temperature:






















nk
qe
TTT
T
II
g
ccRcR
c
oR
11
exp
3
3
0
(5)
In (5), IoR is the reference dark current. The other parameters appeared from (2) to (5) are the electron chargeq,the Boltzman
constant k, the band-gap energy of the PV cell eg, and the diode ideality factor n which is used to adjust the characteristic I − V
curves. The constants in the above equations can be obtained from the data sheet provided by the manufacturer [14].
Cascaded multilevel inverter with separate dc source is proposed in this thesisforsupplyingtheloadwiththesolarPVpanel.It
is assumed that with a proper maximum power point algorithm the output of the PV array is a constant DC source and
simulation is being carried out for 2 level , 3 level, 5 level and 7 level multilevel inverter and the results are being compared.
The multilevel inverters requires too many semiconductor switches and thus its cost gets increased and thus the use of
multilevel inverters are justified by showing the voltage and current burden on each switch and thus it is showed that in spite
of the increased number of switches there will not be much cost difference as the burden on switches gets reduced low rating
semiconductor devices can be used to implement the module. Also the control strategy is very much simple there will not be
much cost difference. Also it is shown that voltageandcurrent total harmonicdistortiongetsreducedonincreasing thenumber
of levels in a multilevel inverter.
3.1 Two level inverter
Figure 4 shows a single phase h bridge inverter having 4 switches. Generally anIGBTisusedasa switchinaninverter.Itisseen
that an R-L load is being connected between the two legs of the inverter. A conventional twolevel inverterusesthetwovoltage
levels at the output of the inverter they are the +V volt and –V volt. For output to be +V volt switch S1 and S2 are closed
together and S3 and S4 are kept open. To obtain –V volt at the output S3 and S4 are closed together and S1 and S2 are kept
open. The switching table of a Two level inverter is shown in table 1. The output waveform of a two level inverter is shown in
figure 5.
Fig. 4 A single phase h bridge inverter

Table 1 Switching Table of Two Level H Bridge Inverter
Fig 5 Output Waveform of a Two Level Inverter
3.2 Three level inverter
By manipulating the switching signals of the h bridge inverter of figure 1, three level inverter can be obtained. A three level
inverter has three level of voltage at the output side namely 0 volt level, +V volt level and –V volt level. The switching table of a
three level inverter is shown in table 2. The output voltage waveform of a three level inverter is shown in figure 6.
Table 2 Switching Table of a Three Level Inverter
Fig 6 Output Waveform of a Three Level Inverter
3.3 Five level inverter
Figure 7 represents the circuit diagram of a five level inverter. It requires two cascaded connecter h level bridge having eight
switches. The output voltage levels are 0 volt, +V/2 volt, -V/2 volt, +V volt and –V volts. The switching sequence to obtain 0 ,
+V/2, -V/2, +V and –V is shown in the table 3. The output waveform of a five level inverter is as shown in the figure 8.
Voltage
level
S1 S2 S3 S4
+V 1 0 0 1
-V 0 1 1 0
Voltage level S1 S2 S3 S4
0 0 0 1 1
+V 1 0 1 0
-V 0 1 1 0

Fig 7 Circuit Diagram of a Five Level Inverter
Table 3 Switching Table of five Level Inverter
Voltage S1 S2 S3 S4 S5 S6 S7 S8
0 0 0 1 1 0 0 1 1
+V/2 1 0 0 1 0 0 1 1
-V/2 0 1 1 0 0 0 1 1
+V 1 0 0 1 1 0 0 1
-V 0 1 1 0 0 1 1 0
Fig 8 Waveform of a 5 Level Inverter
3.4 Seven Level Inverter
Figure 9 represents the circuit diagram of a 7 level inverter. It requires three dc voltage source and 12 switches. The voltage
levels of a 7 level inverter are 0, V/3, 2V/3,V,-V/3,-2V/3 and –V volts. On proper switching these voltage levels at different
instant of time is obtained to obtain the nearly sinusoidal signals. The switchingsequencetoobtainthedesiredvoltagelevelsis
shown in table 4. The output waveform of the 7 level inverter is shown in figure 10.
Fig 9 Circuit Diagram of a 7 Level Inverter

Table 4 Switching Table of a Seven Level Inverter
Volt S1 S2 S3 S4 S5 S6 S7 S8 S9 S10 S11 S12
0 0 0 1 1 0 0 1 1 0 0 1 1
+V/3 1 0 0 1 0 0 1 1 0 0 1 1
-V/3 0 1 1 0 0 0 1 1 0 0 1 1
+2V/3 1 0 0 1 1 0 0 1 0 0 1 1
-2V/3 0 1 0 0 0 1 1 0 0 0 1 1
+V 1 0 0 1 1 0 0 1 1 0 0 1
-V 0 1 1 0 0 1 1 0 0 1 1 0
Fig 10 waveform of a 7 level inverter
3.5 Selective Harmonic Elimination
The basic idea of the selective harmonic elimination is to pre-determine the switching angle for each module to get the
expected waveform of the output [8]. To explain its implementation in the cascaded H-bridge multilevel inverter,one example
of five modules, eleven levels CHB multilevel inverter is shown in Figure 11.
Fig 11 Output waveform of an 11-level cascade inverter

By using Fourier Transform, the output voltage V (ωt) can be expressed as
where n is the harmonic order. Since the waveform is both half wave symmetry and odd symmetry,n=1,3,5,7,....Usually,the
normalized Fourier coefficients of the magnitude are used for further analysis. The normalized magnitude can be obtainedby
dividing Vdc on both sides of equation 4.1. Hence, the normalized Fourier coefficients for each harmonicordercomponentsare
where n = 1, 3, 5, . ... Then by choosing the conducting angle θ1 → θ5 appropriately, it is possible to eliminate some target
harmonic components [8]. Another point need to be mentioned is that the number of harmonic components which can be
eliminated by this modulation method is one less than the numberof theconductinganglessinceonedegreeoffreedomshould
be given to the fundamental components of the waveform. In this case, the number of harmonics that can be eliminated is 4.
Since the triple harmonic would not exist in the line to line voltage, the 5th, 7th, 11th and 13th order harmonics are chosen as
the target harmonics that need to be eliminated in this case. The following equation can be obtained:
where mi is reference modulation index which is defined as mi = Vref 5Vdc . One advantage of this modulation method is that
the inverter is switching at the fundamental frequency which decreases the switching losses. However, the pre-calculation of
the conducting angle requires the solution of non-linear equation. When the level of inverterincreases, the number ofthenon-
linear equations would also be very high. Then the solution for these equations would be inaccurate which may increase the
distortion in the output voltage waveform [9].
3.6 Phase Shifted Pulse Width Modulation
Phase shifted PWM is one of the most commonly used modulation method in CHB multilevel inverter since it is very suitable
for the modularity of the topology. For each module, the reference signal is the same. However, the carrier waveform (usually
triangular waveform) for each module would have a phase shift to ensure the step characteristic of the output voltage. How
many degrees is the phase shift between each module depends on the modulation methodfortheindividual H-bridgeinverter.
If the unipolar modulation method is selected, the phase shift between each module should be 180◦/k to achieve the lowest
output voltage distortion; if the bipolar modulation method is chosen, the phase shift between each module should be 360◦/k
[10], where k is the number of modules. Three modules,sevenlevelsCHBmultilevel inverter withunipolarmodulationmethod
is shown in Figure 12.
Figure 12 Three cell PS-PWM waveform generation

The output voltage of the inverter is as k times as the output voltage of each module which is one advantage ofthismodulation
method since the switching devices need only withstand the voltage of their modules. Moreover, the frequency of the output
voltage has k times as the switching frequency of each module which is beneficial in reducing the conducting losses of the
inverter.
An open loop control structure using Fibonacci series control signal is being implemented in this paper. A sinusoidal signal is
compared with a constant value whose value is determined using the Fibonacci series. From the switchingtablesitisseenthat
the switch in the lower limb is having gate signal such that it is complement of the upper limb gate signal for example gate
signal of S3 which is the lower part of S1 is not of gate signal of S1. Now to obtain the desired signal a sinusoidal signal whose
frequency is equal to 50 Hz is being compared to a constant value signal and gate signal is being generated.
Let the sine wale signal which is being compared with a constant value signal be denoted by F.
For a two pulse inverter there is only one constant value signal whose value is 0. If F is greater than 0 then switch S1 is ON.
If F is lesser than 0 then switch S2 is ON. The gate signals given to S3 and S4 are inverter gate signals of S1 and S2 respectively.
For a 3 level inverter the only difference is that S1 is ON when F is greater than 2 and S2 is on when F is lesser than -2.
For a five level inverter there are 4 more switches. The switching of S1 and S2 are similar to that of a three level inverter.
Switch S5 is ON when F is greater than 5 and switch S6 is on when F is lesser than -5. Switch S7 and S8 are the inverted signals
of S5 and S6 respectively.
For a seven level inverter S9 is On when f is greater than 9 and S10 is ON when F is lesser than -9. Switches S11 and S12 gets
the gate signal of inverted values of S9 and S10 respectively.
Thus with the increase of each bridge the sinusoidal signal F is compared with the constant value which is obtained by
Fibonacci series starting with 2. Such as 2,5,9,14,……. The amplitude of the sinusoidal signal has to be kept in such a manner
that it should be the next number in Fibonacci series after the largest constant value of the constantsignal usedfor controlling.
For example the amplitude of F for 2,3,5 and 7 level must be 2,5,9, 14 respectively.
SIMULATION DIAGRAM AND RESULTS-
Simulation of inverter having different voltage levels are being done is a mat lab simulink using sim power system toolbox.
The simulation diagram of a two level inverter with control signals is being showninfigure13.Themagnitudeofthedcvoltage
used is 230 2 which is the peak value of a sinusoidal signal whose rms vale is 230 Volt.
Fig 13 simulation diagram of a two level inverter
A load whose resistance is 10 Ω and inductance of 5 mili Henry is being connected to the output of the inverter to obtain the
waveform of output voltage and current. Figure 14 shows the output voltage and waveform of a two level inverter.
Fig 14 Output voltage and current of a two level inverter.(yellow line is waveform of voltage and the pink line is
the waveform of the current)

Simulation diagram of a three level inverter with its control structure is being shown in figure 15. The outpul voltage and
current is being shown in figure 16.
Fig 15 Simulation diagram of a three level inverter
Fig 16 Output voltage and current of a three level inverter. (yellow line is waveform of voltage and the pink line is
Simulation diagram of a five level inverter with its control structureisbeingshowninfigure17. Theoutputvoltageandcurrent
is being shown in figure 18. Here the voltage source used is
2
2230 .
Fig 17 Simulation diagram of a five level inverter
Fig 18 Output voltage and current of a five level inverter. (yellow line is waveform of voltage and the pink line is

Simulation diagram of a five level inverter with its control structureisbeingshowninfigure19. Theoutputvoltageandcurrent
is being shown in figure 20. Here the voltage source used is
3
2230 .
Fig 19 Simulation diagram of a seven level inverter
Fig 20 Output voltage and current of a seven level inverter. (yellow line is waveform of voltage and the pink line is
From the results obtained from all levels of inverter the voltage burden, current burden of the switches used, voltage
harmonics and current harmonics of the output is compared in table 5
4. CONCLUSION:-
From the various results obtained from different waveforms of different inverters and comparing the results obtained as
shown in table 5 it is concluded that on increasing the number of voltage levels in an inverter the power quality of the output
obtained goes on increasing the total harmonic distortion of voltage as well as the current waveform is reduced and also
voltage burden on each switch is being reduced to a large extent. On further increasing the voltage levels the output obtained
can be made nearly sinusoidal so as to supply the load with a good power quality if it is being supplied by the photo voltaic
array which is having DC voltage as the output
There are still some improvements which can be added to the system. First of all, it would be very interesting that the energy
storage system such as battery or super-capacitor can be integrated into the system. This will make the system more reliable.
When there is no radiation at all, the system can still provide power from the energy storage system.
5. REFERANCES-
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Electron., vol. 53, no. 4, pp. 1002-1016, Aug. 2006.
[2] Kuang Honghai, Wu Zhengqiu, "Research of super capacitor energy storage system based on DG connected to power
grid" SUPERGEN Conf., Nanjing, China, 2009.

[3] Tang Xisheng "Study on SCES systems used in distributed generation system", Master thesis, Chinese Academy of
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[4] J. S. Lai, F. Z. Peng, "Multilevel Converters- A new Breed of Power Converters" IEEE Transaction on Industrial
Applications, vol. 32, no. 3, pp. 691-697, May/June 1996.
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[6] J. Rodríguez, J. S. Lai, F. Z. Peng, "Multilevel Inverters: A survey of Topologies, Controls, and Application" IEEE
Transaction on Industrial Electronics, vol. 49, no. 4, pp. 724-738, August 2002.
[7] M. Vasiladiotis, "Analysis, Implementation and Experimental Evaluation of Control Systems for a Modular Multilevel
Converter", Master thesis, Royal Institute of Technology, 2009.
[8] L. Tolbert, F. Z. Peng and T. Habetler, "Multilevel converters for large electric drives" IEEE Trans. Ind. Applicat.,vol.35,
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IRJET- Optimal Control of Multilevel Inverter to Minimize Harmonic Distortion in Photovoltaic Power Generating Array

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