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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2479
Modeling and Simulation of PV array in Matlab/Simulink for
comparison of perturb and observe & incremental conductance
algorithms using buck converter
Sandeep Neupane1, Ajay Kumar2
1 M.Tech Scholar (Power electronics and drives), Swami Vivekanand Subharti University, Meerut, India
2 Asst. Prof., EEE Department, SITE, Swami Vivekanand Subharti University, Meerut, India
---------------------------------------------------------------------** *---------------------------------------------------------------------
Abstract - This paper defines modeling of solar PV array
based on single diode PV cell equationsinMATLAB/SIMULINK
in order to compare MPPT tracking techniques using perturb
and observe and incremental conductancealgorithmsmaking
use of a buck converter. A PV array is modeled based on the
electrical characteristics of PV module LG300N1C-G3. MPPT
tracking techniques based on perturb and observe and
incremental conductance algorithmsaremodeledinSimulink.
A buck converter topology is used in Simulink for the
comparison of maximumpowerpointtracking. Thesimulation
results show that tracking method using incremental
conductance algorithm is better than that of perturb and
observe algorithm.
Keywords: Photovoltaic, PV module,PVarray,MPPT, P&O,
INC, buck converter, MATLAB, SIMULINK.
1. INTRODUCTION
Photovoltaic cell is a device based on a semiconductor
material that converts energy of sunlight into electrical
energy.
Due to its low power, it is necessary to combine multiple
cells into series or into parallel, forming a photovoltaic
module and modules are further connected in series or into
parallel with the required values of current and voltage to
form a photovoltaic array. Output parameters of cells are
most affected by environmental conditions, especially by
solar irradiation and also by temperature at the input
modules. Therefore, modeling this device necessarily
requires ambient temperature and solar radiation as input
variables. The output of the model can be voltage, currentor
power of the module. Any changes in the input variables are
reflected by changes on the output.
The common approach is to utilize the electrical equivalent
circuit, which is primarily based on a lightgeneratedcurrent
source connected in parallel to a p-n junction diode. Many
models have been proposed for the simulation of a solar cell
or for a complete photovoltaic (PV) system at various solar
intensities and temperature conditions [1-4].
The power conversion efficiency of solar moduleisverylow.
To increase efficiency of solar module proper impedance
matching is required to increase efficiency of solar module.
Different type of MPPT method has been developed by
researcher in recent year. Every method has its advantage
and disadvantage. MPPT algorithms vary due to simplicity,
efficiency, tracking speed, sensor required and cost. The V-I
characteristics of the solar module is nonlinear and
extremely affected by the solar irradiation andtemperature.
To maximize the output power of solar module, it has to be
operated at fixed value of load resistance. This requires a
separate power converter circuit for the MPPT.
MPPT is an essential component of a photovoltaic system,
extensive research has been exposed in recent years and
many new techniques have been reported in this field [5].
MPPT techniques are generally incorporated in an electric
power conversion system that provides a current or voltage
conversion, filtering and regulations for the conduct of a
variety of loads with electrical grids, batteries and motors.
Several methods to track the maximum power point of a PV
module have been suggested and products using these
methods have been now made commercially available for
consumers [6].
From Figure 1, it is clear that there is only one point where
the solar photovoltaic has a maximum power.
Figure 1: MPP from IV and PV characteristics of PV system
2. MATHEMATICAL MODEL OF PV CELL
The most common and simplest approach to model a PV cell
is using the single diode equivalent circuit as shown in
Figure 2. The equivalent circuit of an ideal PV cell consists of
a current source and a diode connected in anti-parallel with
it. A general model of the solar cell is the combination of
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2480
current source (Iph) connected in anti-parallel toa diode‘D’,
series resistance (Rs) and parallel resistance (Rp or Rsh) [7].
I-V and P-V characteristics of PV cell are shown in Figure 1.
Open circuit voltage (Voc) is the maximum voltage a cell can
generate under open circuit condition at I=0 and the short
circuit current (ISC) is the current that corresponds to short
circuit at V=0. Through the operation, the PV cell generates
maximum power at only one point and this point is called as
Maximum Power Point (MPP). Im, Vm and Pm in the graph are
maximum current, maximum voltage and the maximum
power of the solar cell respectively.
Figure 2: Single diode equivalent circuit of PV Cell
The voltage and current generated by a single PV cell is very
low. So, solar cells are interconnected in a series-parallel
combination to achieve thedesiredpower.Desired voltageis
generated by connecting the solar cells in series and the
desired current is generated by connecting the cells in
parallel. Generally, PV module contains a number of solar
cells connected in series.
Following are the equations that define the model of a PV
module [8-11]:
…………………………………………..... (1)
…………………………………………….. (2)
……………………… (3)
…………………………………. (4)
…………... (5)
…………………………... (6)
…………………………………… (7)
Where
Vt: Thermal voltage in volts
k, q: Boltzmann’s constant (1.38e-23J/K), Electronic charge
(1.6e-19C)
Top, Tref: Operating Temperature of module in Kelvin,
Reference temperature of 250 C
Ish: Shunt current in Ampere
S, Sn: Irradiation in device surface in W/m2, Reference
irradiation of 1kW/m2
Iph, Id: Light generated current in Ampere, Diode current in
Ampere.
Isc, Voc: Short circuit current in Ampere, Open circuit voltage
in Volt
Irs: Reverse saturation current at reference temperature in
Ampere
Is: Diode saturation current in Ampere
ki: Temperature coefficient of short circuit current
Eg, n: Band gap energy of cell (1.12eV ), Diode ideality factor
Rs,Rp: Resistance in series in ohm, Resistance in parallel in
ohm
Ns, Np: Number of modules in series, Number of modules in
parallel
C: Number of cells in module
I, V: Module current in Ampere, Module voltage in Volts
3. MAXIMUM POWER POINT TRACKING
Perturb and observe and Incremental conductance are the
two of the most popular maximum power point tracking
techniques.
3.1 Perturb and Observe (P&O)
The P&O algorithm is also called “hill-climbing”, but both
names refer to the same algorithm depending on how it is
implemented. Hill-climbing involves a perturbation on the
duty cycle of the power converter and P&O a perturbationin
the operating voltage of the DC link between the PV array
and the power converter [12].
In the case of the Hill-climbing, perturbing the duty cycle of
the power converter implies modifying the voltage ofthe DC
link between the PV array and the power converter, so both
names refer to the same technique. In this method, the sign
of the last perturbation and the sign of the last increment in
the power are used to decide what the next perturbation
should be. As can be seen in Figure 1, on the left of the MPP
incrementing the voltage increases the power whereas on
the right decrementing the voltage increases the power. If
there is an increment in the power, the perturbation should
be kept in the same direction and if the power decreases,
then the next perturbation should be in the opposite
direction. Based on thesefacts,thealgorithmisimplemented
[12]. The process is repeated until the MPP is reached. Then
the operating point oscillates around the MPP. A scheme of
the algorithm is shown in Figure 3.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2481
Figure 3: P&O Algorithm
3.2 Incremental Conductance (INC)
The incremental conductance algorithm is based on the fact
that the slope of the curve power vs. voltage (current) of the
PV module is zero at the MPP, positive (negative) on the left
of it and negative (positive) on the right, as can be seen in
Figure 1
 ΔV/ΔP = 0 (ΔI/ΔP = 0 ) at the MPP
 ΔV/ΔP > 0 (ΔI/ΔP < 0) on the left of MPP
 ΔV/ΔP < 0 (ΔI/ΔP > 0) on the right of MPP
By comparing the increment of the power versus the
increment of thevoltage(current)betweentwoconsecutives
samples, the change in the MPP voltagecanbedetermined.A
scheme of the algorithm is shown in Figure 4. Similar
schemes can be found in [12-13].Here also, operating points
oscillates around MPP.
Figure 4: INC Algorithm
4. BUCK CONVERTER
A buck converter, or a standard step down converter, is a
DC/DC converter used to decrease DC voltage. A schematic
of a buck converter can be seen in Figure 5 and consists of
one switch, one diode, one capacitor and one inductor.
Figure 5: Buck converter
The buck converter either store energy in the inductor or
discharge the stored energy to the load, which isdoneintwo
different phases. To store energy, the switch connects the
input voltage to the inductor which results in a positive
voltage over the inductor, this phase is called on-time, ton.
When the switch is disconnected, the positive side of the
inductor is connected to the groundvia a diodewhichresults
in a negative voltage over the inductor. The energy is then
discharged from the inductor to the load, referred to as off-
time, tof f , seen in Figure 6 [14].
Figure 6: Inductor current and voltage of a Standard Buck
Converter
5. MODELING OF SYSTEM IN SIMULINK
Figure 7 shows the block diagram of the system under
consideration.
Figure 7: Block diagram of system
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2482
5.1 Modeling of PV array
The mathematical equations given in section II (equation 1
to equation 6) have been written in Simulink using tags,
constant and Math block. Since a single modulehasNs=Np=1,
this value of Np has been used. The generated current is thus
the difference between Iph and (Id + Ish). Hence, Id is
subtracted from Iph using subtractblock andtheoutputisfed
to controlled current source. The rest of the model has been
drawn as shown in Figure 2 to get Simulink model of
equation 7. In order to model a PV module, circuit based
approach has been used. Several PV modules are connected
in series or parallel to get the PV arrayhavingdesiredoutput
voltage and current. The development of PV array using
mathematical equations and circuit based approach of PV
cell is shown in Figure 8.
Now, the PV array blocks modeled by using PV modules in
series or in parallel are grouped into subsystem toforma PV
array in Simulink that accepts irradiation in W/m2 and
temperature in degree centigrade and provides array
current and voltage that can be measured using current
measurement and voltage measurement block respectively.
The 300 W LG300N1C-G3 solar module is taken as the
reference module for modelling and simulation .The
parameters of the module is given in Table1.
The value of series resistance is small, usually in therangeof
(0-1) Ω while that of parallel resistance is large, usually in
the range of (100-1000) Ω. Similarly, ideality factor is in the
range of (2/3-2). In this paper, the value of Rp, Rs and n are
chosen as 212.8143, 0.31448 and 0.96984 respectively.
Figure 8: Modeling of PV array in Simulink
Table 1: Module Data of LG300N1C-G3 solar module
Module Data STC parameters
(250C,1kW/m2)
Maximum Power 300 W
MPP voltage 32 V
MPP current 9.42 A
Open circuit voltage 39.5 V
Short circuit current 10 A
Number of cells 60
ki 0.03
5.2 MODELING OF MPPT ALGORITHMS
MPPT using incremental conductance algorithm asdepicted
in Figure 4 is modeled in Simulink as shown in Figure 9.
A subsystem is created for PWM generator whose input is
duty cycle obtained from output of MPPTandoutputisPWM
wave.
By creating a separate subsystem, MPPT block is obtained
whose inputs are photovoltaic current and photovoltaic
voltage and whose output is duty cycle. Duty cycle obtained
from MPPT is used to generate PWM wave for converter
switch as shown in Figure 10.
Figure 9: Simulink model of INC MPPT
Figure 10: PWM wave generation in Simulink
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2483
Similarly, MPPT using perturb and observe algorithm as
depicted in Figure 3 is modeled in simulink which is shown
in Figure 11.
Figure 11: Simulink model of P&O MPPT
In both simulink models, memory element is used to hold
and hence compare the previous inputs with the present
input for the functioning of the algorithm. Matlab function is
employed where matlab codes are written for the
implementation of the algorithm.
5.3 MODELING OF BUCK CONVERTER
Buck converter circuit diagram as depicted in Figure 5 is
drawn in Simulink to model DC-DC converter. This circuit is
used as a subsystem to create a buck converter block that
connects positive and negative terminal of PV array and
PWM wave generated by PWM wave generatoroninputside
and positive and negative terminal of load on the output
side.
Figure 12: Simulink model of buck converter
5.4 MODELING OF THE SYSTEM
The above modeled subsystems in Simulink are now
connected to obtain the Simulink model of the system under
consideration. Ten PV modules connected in parallel are
used as a PV array model. MPPT with P&O or INC algorithm
is used in MPPT &PWM block and buck converterisusedasa
dc to dc converter. Figure 13 shows the Simulink model of
the overall system under consideration.
Figure 13: Simulink model of the system under
consideration
A capacitance of 0.025F is used between PV array and buck
converter and the parameters for buck converter used is
L=10e-6H and C=1000e-6 F. A diode and a lead acid battery
of 24 V, 1000 Ah is used as a load of buck converter. Since
the library components used in the model are of Simscape, it
requires powergui block available in library to run the
simulation. Hence, powergui block has been added andused
in continuous mode and ideal switching device. Signal
generator block is used to provide variable input. The
temperature input block is set to 250 C using constant block
while variable input is used for irradiation input.
6. RESULTS AND DISCUSSIONS
The P-V and I-V curves of the photovoltaic array model were
first tested at STC and the result obtained was as shown in
Figure 14.
It can be seen from Figure 14 that the peak power of the
array is 3000 W, open circuit voltage is 39.5 V and short
circuit current is 100 A. If we compare this data with that of
a module as given in Table 1, we see that thepeak powerand
short circuit current has increased by a factor of 10 butopen
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2484
Figure 14: I-V and P-V curve of PV array at STC
Circuit voltage is same as that of a single module. This is
because ten modules have been connected in parallel
because of which voltage rating is same while current rating
is multiplied by a factor of ten. It can be also observed from
the figure that MPP voltage and current of the array are
respectively around 32 V and 950 A thus indicating that the
array is producing the output as per the electrical
characteristics of the single module used.
In order to compare INC and P&O algorithms, following
simulations were performed:-
For the first simulation (Case I), irradiation was varied only
at a point. Irradiation was held constant at 200 W/m2
between 0-0.2 sec. At 0.2 sec, it was increased to 400 W/m2.
After every 0.2 sec, irradiation was increased by 200 W/m2.
Thus, input insolation was varied from 200 to 1000 W/m2
with irradiation changing only at a fixed point and the result
obtained was as shown in Figure 15.
Figure 15: Comparison between INC and P&O (Case I)
The simulation results as seen from Figure 15 shows that
there is no major deviation in results while using both
algorithms for this type of inputirradiation. Thearraypower
as obtained from INC and P&O are completely overlapping
each other. However, on careful observation of the two
curves, it was found that the power curve with INC tracking
method is a bit smoother than that of P&O tracking method.
Figure 16: Comparison between INC and P&O (Case II)
For the second simulation (Case II), irradiation was varied
linearly from 200 to 1000 from 0 to 0.5 sec and again from
1000 to 200 from 0.5 to 1 sec. Similarly, it was varied from
200 -800-200 in next 1 sec , 200 – 600 – 200 in another 1 sec
and 200 – 400 –200 in fourth second and the result obtained
was as shown in Figure 16.
From Figure 16, it can be seen that perturb and observe
algorithm has completely failed to track power while
incremental conductance algorithm has started tracking
from 0.5 sec as the irradiation has changedfrom1000to 200
W/m2.
For the third simulation (Case III), insolation was varied
from 0 – 1000 at t=0.2 sec, 1000 – 200 at t=0.4 sec and again
from 200 – 1000 at t = 0.5 sec and the result obtained was as
shown in Figure 17.
Figure 17: Comparison between INC and P&O (Case III)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2485
It can be seen from Figure 17 that both incremental
conductance algorithm and perturb and observe algorithm
has started tracking at 0.2 sec. However, when the input is
constant after 0.5 sec, incremental conductance algorithm
has reached steady state value earlier than perturb and
observe algorithm.
For the fourth simulation (Case IV) , the irradiation was
varied rapidly between 200 - 1000 -200 in the first one
second, 200 – 1000 from t= 1 to t=2 seconds, 1000 – 600
from t=2 to t=2.5 seconds and from 600 – 1000 from t= 2.5
to t= 4 seconds and fixed at 1000 from t= 4 to t=5 seconds.
The result obtained was as shown in Figure 18.
Figure 18: Comparison between INC and P&O (Case IV)
It can be clearly seen from Figure 18 that incremental
conductance algorithm has started tracking at t= 0.5 second
where input irradiation has been varied between 1000 to
200 W/m2. On the other hand, perturb and observe
algorithm has startedtrackingjustafterthreesecondswhere
input irradiation has been varied between 600 to 1000
W/m2. The output power from both algorithms is sameafter
three seconds.
From each of the cases discussed above, the incremental
conductance tracking method has proved either equal or
better than the perturb and observe tracking method.
7. CONCLUSION
This paper has presented a photovoltaic array modeled
using Matlab/Simulink to compare MPPT tracking
techniques using P&O and INC algorithms. PV module has
been modeled by using its equivalent circuit and the
equations involved, for the system simulation. Using
datasheet of LG300N1C-G3 solar module, the PVmodule has
been developed and by connecting modules in parallel, PV
array has been developed and simulated using Simulink of
Matlab R2016b software package. MPPT tracking
techniques has been modeled using P&O andINCalgorithms
and buck converter topology has been used. The simulation
results has shown that incremental conductance algorithm
provides faster, better dynamic response and more reliable
tracking methodcomparedtoperturbandobservealgorithm
when both are subjected to rapidly changing irradiation
level.
REFERENCES
[1] J.A.Gow; C.D Manning; "Development of a photovoltaic
array model for use in power-electronics simulation
studies," Electric Power Applications,IEEProceedings -,
vol.146, no.2, pp.193-200, Mar 1999.
[2] S.Etienne; T. Alberto and S. Mikhaïl; “Explicit model of
photovoltaic panels to determine voltages and currents
at the maximum power point”. Sol Energy 2011;85(5),
pp. 713-22.
[3] T.H.Liang. “Insolation-oriented model of photovoltaic
module using Matlab/simulink”. Sol Energy2010;84(7),
pp.1318-26.
[4] I.Kashif; S. Zainal and T. Hamed. “Simple, fast and
accurate two diode model forphotovoltaicmodules”.Sol
Energy Mater Sol Cells 2011;95(2), pp. 586-94.
[5] Y.H.Chang and C.Y. Chang, "A Maximum Power Point
Tracking of PV System by Scaling Fuzzy Control,"
presented at International Multi Conference of
Engineers and Computer Scientists, HongKong, 2010.
[6] S.Mekhilef, "Performance of grid connected inverter
with maximum power point tracker and power factor
control," International Journal of Power Electronics,
vol.1, pp. 49-62.
[7] M. G. Villalva, J. R. Gazoli, and E. R. Filho,
“Comprehensive approach to modeling and simulation
of photovoltaic arrays,”IEEE Trans. on power Electron.
vol.24, no.5, pp.1198-1208, May 2009.
[8] S. S. Mohammed, “Modeling and simulation of
photovoltaic module using matlab/simulink”
International Journal of Chemical and Environmental
Engineering, vol. 2, no. 5, pp. 350–355, 2011.
[9] S. Gomathy, S. Saravanan, and D. S. Thangavel, “Design
and implementation of maximum power point tracking
algorithm for a standalone pv system,” International
journal of scientific and engineering research, vol. 3, no.
3, 2012.
[10] A. Grama, M. Dan and E. Lázár, "Photovoltaic panel
model using Matlab," 2016 39th International Spring
Seminar on Electronics Technology (ISSE), Pilsen,2016,
pp. 322-327.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2486
[11] P. Suskis and I. Galkin, "Enhanced photovoltaic
panel model for MATLAB-simulink environment
considering solarcell junctioncapacitance," IECON 2013
- 39th Annual Conference of the IEEE Industrial
Electronics Society, Vienna, 2013, pp. 1613-1618.
[12] T. Esram, P.L. Chapman, "Comparison of
Photovoltaic Array Maximum Power Point Tracking
Techniques," IEEE Transactions on Energy Conversion,
vol. 22, no. 2, pp. 439449, June 2007.
[13] S. Jain, V. Agarwal, "Comparison of the performance
of maximum power point tracking schemes applied to
single-stage grid-connected photovoltaic systems,"
Electric Power Applications, IET, vol. 1, no. 5, pp. 753-
762, Sept. 2007.
[14] N. Mohan, T. M. Undeland, W. P. Robbins, “Power
Electronics: Converters, Applications, and Design”, 2nd
ed., John Wiley & Sons, New York, 1995.

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Modeling and Simulation of PV Array in Matlab/Simulink for Comparison of Perturb and Observe & Incremental Conductance Algorithms using Buck Converter

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2479 Modeling and Simulation of PV array in Matlab/Simulink for comparison of perturb and observe & incremental conductance algorithms using buck converter Sandeep Neupane1, Ajay Kumar2 1 M.Tech Scholar (Power electronics and drives), Swami Vivekanand Subharti University, Meerut, India 2 Asst. Prof., EEE Department, SITE, Swami Vivekanand Subharti University, Meerut, India ---------------------------------------------------------------------** *--------------------------------------------------------------------- Abstract - This paper defines modeling of solar PV array based on single diode PV cell equationsinMATLAB/SIMULINK in order to compare MPPT tracking techniques using perturb and observe and incremental conductancealgorithmsmaking use of a buck converter. A PV array is modeled based on the electrical characteristics of PV module LG300N1C-G3. MPPT tracking techniques based on perturb and observe and incremental conductance algorithmsaremodeledinSimulink. A buck converter topology is used in Simulink for the comparison of maximumpowerpointtracking. Thesimulation results show that tracking method using incremental conductance algorithm is better than that of perturb and observe algorithm. Keywords: Photovoltaic, PV module,PVarray,MPPT, P&O, INC, buck converter, MATLAB, SIMULINK. 1. INTRODUCTION Photovoltaic cell is a device based on a semiconductor material that converts energy of sunlight into electrical energy. Due to its low power, it is necessary to combine multiple cells into series or into parallel, forming a photovoltaic module and modules are further connected in series or into parallel with the required values of current and voltage to form a photovoltaic array. Output parameters of cells are most affected by environmental conditions, especially by solar irradiation and also by temperature at the input modules. Therefore, modeling this device necessarily requires ambient temperature and solar radiation as input variables. The output of the model can be voltage, currentor power of the module. Any changes in the input variables are reflected by changes on the output. The common approach is to utilize the electrical equivalent circuit, which is primarily based on a lightgeneratedcurrent source connected in parallel to a p-n junction diode. Many models have been proposed for the simulation of a solar cell or for a complete photovoltaic (PV) system at various solar intensities and temperature conditions [1-4]. The power conversion efficiency of solar moduleisverylow. To increase efficiency of solar module proper impedance matching is required to increase efficiency of solar module. Different type of MPPT method has been developed by researcher in recent year. Every method has its advantage and disadvantage. MPPT algorithms vary due to simplicity, efficiency, tracking speed, sensor required and cost. The V-I characteristics of the solar module is nonlinear and extremely affected by the solar irradiation andtemperature. To maximize the output power of solar module, it has to be operated at fixed value of load resistance. This requires a separate power converter circuit for the MPPT. MPPT is an essential component of a photovoltaic system, extensive research has been exposed in recent years and many new techniques have been reported in this field [5]. MPPT techniques are generally incorporated in an electric power conversion system that provides a current or voltage conversion, filtering and regulations for the conduct of a variety of loads with electrical grids, batteries and motors. Several methods to track the maximum power point of a PV module have been suggested and products using these methods have been now made commercially available for consumers [6]. From Figure 1, it is clear that there is only one point where the solar photovoltaic has a maximum power. Figure 1: MPP from IV and PV characteristics of PV system 2. MATHEMATICAL MODEL OF PV CELL The most common and simplest approach to model a PV cell is using the single diode equivalent circuit as shown in Figure 2. The equivalent circuit of an ideal PV cell consists of a current source and a diode connected in anti-parallel with it. A general model of the solar cell is the combination of
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2480 current source (Iph) connected in anti-parallel toa diode‘D’, series resistance (Rs) and parallel resistance (Rp or Rsh) [7]. I-V and P-V characteristics of PV cell are shown in Figure 1. Open circuit voltage (Voc) is the maximum voltage a cell can generate under open circuit condition at I=0 and the short circuit current (ISC) is the current that corresponds to short circuit at V=0. Through the operation, the PV cell generates maximum power at only one point and this point is called as Maximum Power Point (MPP). Im, Vm and Pm in the graph are maximum current, maximum voltage and the maximum power of the solar cell respectively. Figure 2: Single diode equivalent circuit of PV Cell The voltage and current generated by a single PV cell is very low. So, solar cells are interconnected in a series-parallel combination to achieve thedesiredpower.Desired voltageis generated by connecting the solar cells in series and the desired current is generated by connecting the cells in parallel. Generally, PV module contains a number of solar cells connected in series. Following are the equations that define the model of a PV module [8-11]: …………………………………………..... (1) …………………………………………….. (2) ……………………… (3) …………………………………. (4) …………... (5) …………………………... (6) …………………………………… (7) Where Vt: Thermal voltage in volts k, q: Boltzmann’s constant (1.38e-23J/K), Electronic charge (1.6e-19C) Top, Tref: Operating Temperature of module in Kelvin, Reference temperature of 250 C Ish: Shunt current in Ampere S, Sn: Irradiation in device surface in W/m2, Reference irradiation of 1kW/m2 Iph, Id: Light generated current in Ampere, Diode current in Ampere. Isc, Voc: Short circuit current in Ampere, Open circuit voltage in Volt Irs: Reverse saturation current at reference temperature in Ampere Is: Diode saturation current in Ampere ki: Temperature coefficient of short circuit current Eg, n: Band gap energy of cell (1.12eV ), Diode ideality factor Rs,Rp: Resistance in series in ohm, Resistance in parallel in ohm Ns, Np: Number of modules in series, Number of modules in parallel C: Number of cells in module I, V: Module current in Ampere, Module voltage in Volts 3. MAXIMUM POWER POINT TRACKING Perturb and observe and Incremental conductance are the two of the most popular maximum power point tracking techniques. 3.1 Perturb and Observe (P&O) The P&O algorithm is also called “hill-climbing”, but both names refer to the same algorithm depending on how it is implemented. Hill-climbing involves a perturbation on the duty cycle of the power converter and P&O a perturbationin the operating voltage of the DC link between the PV array and the power converter [12]. In the case of the Hill-climbing, perturbing the duty cycle of the power converter implies modifying the voltage ofthe DC link between the PV array and the power converter, so both names refer to the same technique. In this method, the sign of the last perturbation and the sign of the last increment in the power are used to decide what the next perturbation should be. As can be seen in Figure 1, on the left of the MPP incrementing the voltage increases the power whereas on the right decrementing the voltage increases the power. If there is an increment in the power, the perturbation should be kept in the same direction and if the power decreases, then the next perturbation should be in the opposite direction. Based on thesefacts,thealgorithmisimplemented [12]. The process is repeated until the MPP is reached. Then the operating point oscillates around the MPP. A scheme of the algorithm is shown in Figure 3.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2481 Figure 3: P&O Algorithm 3.2 Incremental Conductance (INC) The incremental conductance algorithm is based on the fact that the slope of the curve power vs. voltage (current) of the PV module is zero at the MPP, positive (negative) on the left of it and negative (positive) on the right, as can be seen in Figure 1  ΔV/ΔP = 0 (ΔI/ΔP = 0 ) at the MPP  ΔV/ΔP > 0 (ΔI/ΔP < 0) on the left of MPP  ΔV/ΔP < 0 (ΔI/ΔP > 0) on the right of MPP By comparing the increment of the power versus the increment of thevoltage(current)betweentwoconsecutives samples, the change in the MPP voltagecanbedetermined.A scheme of the algorithm is shown in Figure 4. Similar schemes can be found in [12-13].Here also, operating points oscillates around MPP. Figure 4: INC Algorithm 4. BUCK CONVERTER A buck converter, or a standard step down converter, is a DC/DC converter used to decrease DC voltage. A schematic of a buck converter can be seen in Figure 5 and consists of one switch, one diode, one capacitor and one inductor. Figure 5: Buck converter The buck converter either store energy in the inductor or discharge the stored energy to the load, which isdoneintwo different phases. To store energy, the switch connects the input voltage to the inductor which results in a positive voltage over the inductor, this phase is called on-time, ton. When the switch is disconnected, the positive side of the inductor is connected to the groundvia a diodewhichresults in a negative voltage over the inductor. The energy is then discharged from the inductor to the load, referred to as off- time, tof f , seen in Figure 6 [14]. Figure 6: Inductor current and voltage of a Standard Buck Converter 5. MODELING OF SYSTEM IN SIMULINK Figure 7 shows the block diagram of the system under consideration. Figure 7: Block diagram of system
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2482 5.1 Modeling of PV array The mathematical equations given in section II (equation 1 to equation 6) have been written in Simulink using tags, constant and Math block. Since a single modulehasNs=Np=1, this value of Np has been used. The generated current is thus the difference between Iph and (Id + Ish). Hence, Id is subtracted from Iph using subtractblock andtheoutputisfed to controlled current source. The rest of the model has been drawn as shown in Figure 2 to get Simulink model of equation 7. In order to model a PV module, circuit based approach has been used. Several PV modules are connected in series or parallel to get the PV arrayhavingdesiredoutput voltage and current. The development of PV array using mathematical equations and circuit based approach of PV cell is shown in Figure 8. Now, the PV array blocks modeled by using PV modules in series or in parallel are grouped into subsystem toforma PV array in Simulink that accepts irradiation in W/m2 and temperature in degree centigrade and provides array current and voltage that can be measured using current measurement and voltage measurement block respectively. The 300 W LG300N1C-G3 solar module is taken as the reference module for modelling and simulation .The parameters of the module is given in Table1. The value of series resistance is small, usually in therangeof (0-1) Ω while that of parallel resistance is large, usually in the range of (100-1000) Ω. Similarly, ideality factor is in the range of (2/3-2). In this paper, the value of Rp, Rs and n are chosen as 212.8143, 0.31448 and 0.96984 respectively. Figure 8: Modeling of PV array in Simulink Table 1: Module Data of LG300N1C-G3 solar module Module Data STC parameters (250C,1kW/m2) Maximum Power 300 W MPP voltage 32 V MPP current 9.42 A Open circuit voltage 39.5 V Short circuit current 10 A Number of cells 60 ki 0.03 5.2 MODELING OF MPPT ALGORITHMS MPPT using incremental conductance algorithm asdepicted in Figure 4 is modeled in Simulink as shown in Figure 9. A subsystem is created for PWM generator whose input is duty cycle obtained from output of MPPTandoutputisPWM wave. By creating a separate subsystem, MPPT block is obtained whose inputs are photovoltaic current and photovoltaic voltage and whose output is duty cycle. Duty cycle obtained from MPPT is used to generate PWM wave for converter switch as shown in Figure 10. Figure 9: Simulink model of INC MPPT Figure 10: PWM wave generation in Simulink
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2483 Similarly, MPPT using perturb and observe algorithm as depicted in Figure 3 is modeled in simulink which is shown in Figure 11. Figure 11: Simulink model of P&O MPPT In both simulink models, memory element is used to hold and hence compare the previous inputs with the present input for the functioning of the algorithm. Matlab function is employed where matlab codes are written for the implementation of the algorithm. 5.3 MODELING OF BUCK CONVERTER Buck converter circuit diagram as depicted in Figure 5 is drawn in Simulink to model DC-DC converter. This circuit is used as a subsystem to create a buck converter block that connects positive and negative terminal of PV array and PWM wave generated by PWM wave generatoroninputside and positive and negative terminal of load on the output side. Figure 12: Simulink model of buck converter 5.4 MODELING OF THE SYSTEM The above modeled subsystems in Simulink are now connected to obtain the Simulink model of the system under consideration. Ten PV modules connected in parallel are used as a PV array model. MPPT with P&O or INC algorithm is used in MPPT &PWM block and buck converterisusedasa dc to dc converter. Figure 13 shows the Simulink model of the overall system under consideration. Figure 13: Simulink model of the system under consideration A capacitance of 0.025F is used between PV array and buck converter and the parameters for buck converter used is L=10e-6H and C=1000e-6 F. A diode and a lead acid battery of 24 V, 1000 Ah is used as a load of buck converter. Since the library components used in the model are of Simscape, it requires powergui block available in library to run the simulation. Hence, powergui block has been added andused in continuous mode and ideal switching device. Signal generator block is used to provide variable input. The temperature input block is set to 250 C using constant block while variable input is used for irradiation input. 6. RESULTS AND DISCUSSIONS The P-V and I-V curves of the photovoltaic array model were first tested at STC and the result obtained was as shown in Figure 14. It can be seen from Figure 14 that the peak power of the array is 3000 W, open circuit voltage is 39.5 V and short circuit current is 100 A. If we compare this data with that of a module as given in Table 1, we see that thepeak powerand short circuit current has increased by a factor of 10 butopen
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2484 Figure 14: I-V and P-V curve of PV array at STC Circuit voltage is same as that of a single module. This is because ten modules have been connected in parallel because of which voltage rating is same while current rating is multiplied by a factor of ten. It can be also observed from the figure that MPP voltage and current of the array are respectively around 32 V and 950 A thus indicating that the array is producing the output as per the electrical characteristics of the single module used. In order to compare INC and P&O algorithms, following simulations were performed:- For the first simulation (Case I), irradiation was varied only at a point. Irradiation was held constant at 200 W/m2 between 0-0.2 sec. At 0.2 sec, it was increased to 400 W/m2. After every 0.2 sec, irradiation was increased by 200 W/m2. Thus, input insolation was varied from 200 to 1000 W/m2 with irradiation changing only at a fixed point and the result obtained was as shown in Figure 15. Figure 15: Comparison between INC and P&O (Case I) The simulation results as seen from Figure 15 shows that there is no major deviation in results while using both algorithms for this type of inputirradiation. Thearraypower as obtained from INC and P&O are completely overlapping each other. However, on careful observation of the two curves, it was found that the power curve with INC tracking method is a bit smoother than that of P&O tracking method. Figure 16: Comparison between INC and P&O (Case II) For the second simulation (Case II), irradiation was varied linearly from 200 to 1000 from 0 to 0.5 sec and again from 1000 to 200 from 0.5 to 1 sec. Similarly, it was varied from 200 -800-200 in next 1 sec , 200 – 600 – 200 in another 1 sec and 200 – 400 –200 in fourth second and the result obtained was as shown in Figure 16. From Figure 16, it can be seen that perturb and observe algorithm has completely failed to track power while incremental conductance algorithm has started tracking from 0.5 sec as the irradiation has changedfrom1000to 200 W/m2. For the third simulation (Case III), insolation was varied from 0 – 1000 at t=0.2 sec, 1000 – 200 at t=0.4 sec and again from 200 – 1000 at t = 0.5 sec and the result obtained was as shown in Figure 17. Figure 17: Comparison between INC and P&O (Case III)
  • 7. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2485 It can be seen from Figure 17 that both incremental conductance algorithm and perturb and observe algorithm has started tracking at 0.2 sec. However, when the input is constant after 0.5 sec, incremental conductance algorithm has reached steady state value earlier than perturb and observe algorithm. For the fourth simulation (Case IV) , the irradiation was varied rapidly between 200 - 1000 -200 in the first one second, 200 – 1000 from t= 1 to t=2 seconds, 1000 – 600 from t=2 to t=2.5 seconds and from 600 – 1000 from t= 2.5 to t= 4 seconds and fixed at 1000 from t= 4 to t=5 seconds. The result obtained was as shown in Figure 18. Figure 18: Comparison between INC and P&O (Case IV) It can be clearly seen from Figure 18 that incremental conductance algorithm has started tracking at t= 0.5 second where input irradiation has been varied between 1000 to 200 W/m2. On the other hand, perturb and observe algorithm has startedtrackingjustafterthreesecondswhere input irradiation has been varied between 600 to 1000 W/m2. The output power from both algorithms is sameafter three seconds. From each of the cases discussed above, the incremental conductance tracking method has proved either equal or better than the perturb and observe tracking method. 7. CONCLUSION This paper has presented a photovoltaic array modeled using Matlab/Simulink to compare MPPT tracking techniques using P&O and INC algorithms. PV module has been modeled by using its equivalent circuit and the equations involved, for the system simulation. Using datasheet of LG300N1C-G3 solar module, the PVmodule has been developed and by connecting modules in parallel, PV array has been developed and simulated using Simulink of Matlab R2016b software package. MPPT tracking techniques has been modeled using P&O andINCalgorithms and buck converter topology has been used. The simulation results has shown that incremental conductance algorithm provides faster, better dynamic response and more reliable tracking methodcomparedtoperturbandobservealgorithm when both are subjected to rapidly changing irradiation level. REFERENCES [1] J.A.Gow; C.D Manning; "Development of a photovoltaic array model for use in power-electronics simulation studies," Electric Power Applications,IEEProceedings -, vol.146, no.2, pp.193-200, Mar 1999. [2] S.Etienne; T. Alberto and S. Mikhaïl; “Explicit model of photovoltaic panels to determine voltages and currents at the maximum power point”. Sol Energy 2011;85(5), pp. 713-22. [3] T.H.Liang. “Insolation-oriented model of photovoltaic module using Matlab/simulink”. Sol Energy2010;84(7), pp.1318-26. [4] I.Kashif; S. Zainal and T. Hamed. “Simple, fast and accurate two diode model forphotovoltaicmodules”.Sol Energy Mater Sol Cells 2011;95(2), pp. 586-94. [5] Y.H.Chang and C.Y. Chang, "A Maximum Power Point Tracking of PV System by Scaling Fuzzy Control," presented at International Multi Conference of Engineers and Computer Scientists, HongKong, 2010. [6] S.Mekhilef, "Performance of grid connected inverter with maximum power point tracker and power factor control," International Journal of Power Electronics, vol.1, pp. 49-62. [7] M. G. Villalva, J. R. Gazoli, and E. R. Filho, “Comprehensive approach to modeling and simulation of photovoltaic arrays,”IEEE Trans. on power Electron. vol.24, no.5, pp.1198-1208, May 2009. [8] S. S. Mohammed, “Modeling and simulation of photovoltaic module using matlab/simulink” International Journal of Chemical and Environmental Engineering, vol. 2, no. 5, pp. 350–355, 2011. [9] S. Gomathy, S. Saravanan, and D. S. Thangavel, “Design and implementation of maximum power point tracking algorithm for a standalone pv system,” International journal of scientific and engineering research, vol. 3, no. 3, 2012. [10] A. Grama, M. Dan and E. Lázár, "Photovoltaic panel model using Matlab," 2016 39th International Spring Seminar on Electronics Technology (ISSE), Pilsen,2016, pp. 322-327.
  • 8. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2486 [11] P. Suskis and I. Galkin, "Enhanced photovoltaic panel model for MATLAB-simulink environment considering solarcell junctioncapacitance," IECON 2013 - 39th Annual Conference of the IEEE Industrial Electronics Society, Vienna, 2013, pp. 1613-1618. [12] T. Esram, P.L. Chapman, "Comparison of Photovoltaic Array Maximum Power Point Tracking Techniques," IEEE Transactions on Energy Conversion, vol. 22, no. 2, pp. 439449, June 2007. [13] S. Jain, V. Agarwal, "Comparison of the performance of maximum power point tracking schemes applied to single-stage grid-connected photovoltaic systems," Electric Power Applications, IET, vol. 1, no. 5, pp. 753- 762, Sept. 2007. [14] N. Mohan, T. M. Undeland, W. P. Robbins, “Power Electronics: Converters, Applications, and Design”, 2nd ed., John Wiley & Sons, New York, 1995.