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i
A SEMINAR REPORT ON
MPPT Technology
Submitted in partial fulfillment of the requirement of the award of the degree
Of
BACHELOR OF TECHNOLOGY
IN
Electronics and Communication Engineering
Submitted To Submitted by
Mr. Rohit Negi Manish Barthwal
Mr. Ajay Kumar (142107)
ECE-3rd
year
DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING
G B PANT ENGINEERING COLLEGE PAURI GARHWAL (UTTARAKHAND) INDIA
ii
ACKNOWLEDGMENT
I would like to thank respected Mr. Rohit Negi and Mr. Ajay Kumar for giving me
such a wonderful opportunity to expand my knowledge for my own branch and giving
me guidelines to present a seminar report. It helped me a lot to realize of what we
study for.
Secondly, I would like to thank my parents who patiently helped me as i went through
my work and helped to modify and eliminate some of the irrelevant or un-necessary
stuffs.
Thirdly, I would like to thank my friends who helped me to make my work more
organized and well-stacked till the end.
Next, I would thank Microsoft for developing such a wonderful tool like MS Word. It
helped my work a lot to remain error-free.
Last but clearly not the least, I would thank The Almighty for giving me strength to
complete my report on time.
iii
ABSTRACT
Due to rapid growth in the semiconductor and power electronics techniques,
PV energy is of increasing interest in electrical power applications. Photovoltaic (PV)
energy is the most important energy resource since it is clean, pollution free, and
inexhaustible It is important to operate PV energy conversion systems near the
maximum power point to increase the output efficiency of PV arrays. The output
power of PV arrays is always changing with weather conditions, i.e., solar irradiation
and atmospheric temperature. Therefore, a MPPT control to extract maximum power
from the PV arrays at real time becomes indispensable in PV generation system. In
recent years, a large number of techniques have been proposed for tracking the
maximum power point (MPP). Maximum power point tracking (MPPT) is used in
photovoltaic (PV) systems to maximize the photovoltaic array output power,
irrespective of the temperature and radiation conditions and of the load electrical
characteristics the PV array output power is used to directly control the dc/dc
converter, thus reducing the complexity of the system. The resulting system has high-
efficiency; lower-cost this paper proposes a maximum-PowerPoint tracking (MPPT)
method with a simple algorithm for photovoltaic (PV) power generation systems. The
method is based on use of a Incremental conductance of the PV to determine an
optimum operating current for the maximum output power. This work proposes on
Investigation of Incremental conductance Based maximum Power Point Tracking for
Photovoltaic System, to have the advantages of low frequency switching.
iv
TABLE OF CONTENTS
ACKNOWLEDGEMENT ii
ABSTRACT iii
TABLE OF CONTENTS iv
1. INTRODUCTION 1
2. SOLAR CELL MODELING
2.1) MODELING OF SOLAR CELL 2
2.2) EFFECT OF IRRADIATION 4
2.3) EFFECT OF TEMPERATURE 5
3. BOOST CONVERTER
3.1) BOOST CONVERTER 7
3.2) MODES OF OPERATION 7
3.3) WAVEFORMS 8
4. MAXIMUM POWER POINT TRACKING
4.1) MAXIMUM POWER POINT TRACKING 9
4.2) METHODS OF MPPT 9
4.3) FLOW CHART OF ALGORITHMS 13
5. CONCLUSION & FUTURE WORK
5.1) CONCLUSION 16
5.2) FUTURE WORK 16
6. REFERENCE 17
1
INTRODUCTION
One of the major concerns in the power sector is the day-to-day increasing
power demand but the unavailability of enough resources to meet the power demand
using the conventional energy sources. Demand has increased for renewable sources
of energy to be utilized along with conventional systems to meet the energy demand.
Renewable sources like wind energy and solar energy are the prime energy sources
which are being utilized in this regard. The continuous use of fossil fuels has caused
the fossil fuel deposit to be reduced and has drastically affected the environment
depleting the biosphere and cumulatively adding to global warming.
Solar energy is abundantly available that has made it possible to harvest it and
utilize it properly. Solar energy can be a standalone generating unit or can be a grid
connected generating unit depending on the availability of a grid nearby. Thus it can
be used to power rural areas where the availability of grids is very low. Another
advantage of using solar energy is the portable operation whenever wherever
necessary.
In order to tackle the present energy crisis one has to develop an efficient manner in
which power has to be extracted from the incoming solar radiation. The power
conversion mechanisms have been greatly reduced in size in the past few years. The
development in power electronics and material science has helped engineers to come
up very small but powerful systems to withstand the high power demand. But the
disadvantage of these systems is the increased power density. Trend has set in for the
use of multi-input converter units that can effectively handle the voltage fluctuations.
But due to high production cost and the low efficiency of these systems they can
hardly compete in the competitive markets as a prime power generation source.
The constant increase in the development of the solar cells manufacturing technology
would definitely make the use of these technologies possible on a wider basis than
what the scenario is presently. The use of the newest power control mechanisms called
the Maximum Power Point Tracking (MPPT) algorithms has led to the increase in the
efficiency of operation of the solar modules and thus is effective in the field of
utilization of renewable sources of energy.
2
SOLAR CELL MODELING
2.1 MODELLING OF SOLAR CELL
A solar cell is the building block of a solar panel. A photovoltaic module is formed by
connecting many solar cells in series and parallel. Considering only a single solar cell;
it can be modeled by utilizing a current source, a diode and two resistors. This model
is known as a single diode model of solar cell. Two diode models are also available
but only single diode model is considered here [1], [2], [4], [7], [9] and [10].
Figure 2: Single diode model of a solar cell
Fig.1: MPPT block scheme
3
The characteristic equation for a photovoltaic cell is given by [1], [2], [4], [7], [9] and [10],
I & V : Cell output current and voltage;
Ios : Cell reverse saturation current;
T : Cell temperature in Celsius;
k : Boltzmann's constant, 1.38 * 10-19 J/K;
q : Electron charge, 1.6*10-23 C;
Ki : Short circuit current temperature coefficient at Iscr;
lambda : Solar irradiation in W/m^2;
Iscr : Short circuit current at 25 degree Celsius;
Ilg : Light-generated current;
Ego : Band gap for silicon;
A : Ideality factor;
Tr : Reference temperature;
Ior : Cell saturation current at Tr;
Rsh : Shunt resistance;
Rs : Series resistance;
The characteristic equation of a solar module is dependent on the number of cells in
parallel and number of cells in series. It is observed from experimental results that the
current variation is less dependent on the shunt resistance and is more dependent on
the series resistance [7].
4
The I-V and P-V curves for a solar cell are given in the following figure. It can be
seen that the cell operates as a constant current source at low values of operating
voltages and a constant voltage source at low values of operating current.
Figure 3: P-V I-V curve of a solar cell at given temperature and solar irradiation
2.2 EFFECT OF VARIATION OF SOLAR IRRADIATION
The P-V and I-V curves of a solar cell are highly dependent on the solar irradiation
values. The solar irradiation as a result of the environmental changes keeps on
fluctuating, but control mechanisms are available that can track this change and can
alter the working of the solar cell to meet the required load demands. Higher is the
solar irradiation, higher would be the solar input to the solar cell and hence power
magnitude would increase for the same voltage value. With increase in the solar
irradiation the open circuit voltage increases. This is due to the fact that, when more
sunlight incidents on to the solar cell, the electrons are supplied with higher excitation
energy, thereby increasing the electron mobility and thus more power is generated [7]
and [10].
5
Figure 4: Variation of P-V curve with solar irradiation
Figure 5: Variation of I-V curve with solar irradiation
2.3 EFFECT OF VARIATION OF TEMPERATURE
On the contrary the temperature increase around the solar cell has a negative impact
on the power generation capability. Increase in temperature is accompanied by a
decrease in the open circuit voltage value. Increase in temperature causes increase in
the band gap of the material and thus more energy is required to cross this barrier.
Thus the efficiency of the solar cell is reduced [7] and [10].
6
Figure 6: Variation of P-V curve with temperature
Figure 7: Variation of I-V with temperature
7
BOOST CONVERTER
3.1 BOOST CONVERTER
Boost converter steps up the input voltage magnitude to a required output voltage
magnitude without the use of a transformer. The main components of a boost
converter are an inductor, a diode and a high frequency switch. These in a co-
ordinated manner supply power to the load at a voltage greater than the input voltage
magnitude. The control strategy lies in the manipulation of the duty cycle of the
switch which causes the voltage change [11] and [12].
Figure 8: A boost converter
3.2 MODES OF OPERATION
There are two modes of operation of a boost converter. Those are based on the closing
and opening of the switch. The first mode is when the switch is closed; this is known
as the charging mode of operation. The second mode is when the switch is open; this
is known as the discharging mode of operation [12].
3.2.1 Charging Mode
In this mode of operation; the switch is closed and the inductor is charged by the
source through the switch. The charging current is exponential in nature but for
simplicity is assumed to be linearly varying [11]. The diode restricts the flow of
8
current from the source to the load and the demand of the load is met by the
discharging of the capacitor.
3.2.2Discharging Mode
In this mode of operation; the switch is open and the diode is forward biased [11]. The
inductor now discharges and together with the source charges the capacitor and meets
the load demands. The load current variation is very small and in many cases is
assumed constant throughout the operation.
3.3 WAVEFORMS
Figure 9: Waveforms of boost converter
9
MAXIMUM POWER POINT TRACKING
4.1 MAXIMUM POWER POINT TRACKING
The efficiency of a solar cell is very low. In order to increase the efficiency, methods
are to be undertaken to match the source and load properly. One such method is the
Maximum Power Point Tracking (MPPT). This is a technique used to obtain the
maximum possible power from a varying source. In photovoltaic systems the I-V
curve is non-linear, thereby making it difficult to be used to power a certain load. This
is done by utilizing a boost converter whose duty cycle is varied by using a mppt
algorithm. Few of the many algorithms are listed below [3], [4], [5] and [8].
A boost converter is used on the load side and a solar panel is used to power this
converter.
4.2 METHODS FOR MPPT
There are many methods used for maximum power point tracking a few are listed
below:
• Perturb and Observe method
• Incremental Conductance method
• Parasitic Capacitance method
• Constant Voltage method
• Constant Current method
4.2.1 Perturb and Observe method
This method is the most common. In this method very less number of sensors are
utilized [5] and [6]. The operating voltage is sampled and the algorithm changes the
operating voltage in the required direction and samples ݀ܲ/ܸ݀. If ݀ܲ/ܸ݀ is positive,
then the algorithm increases the voltage value towards the MPP until ݀ܲ/ܸ݀ is
negative. This iteration is continued until the algorithm finally reaches the MPP. This
10
algorithm is not suitable when the variation in the solar irradiation is high. The voltage
never actually reaches an exact value but perturbs around the maximum power point
(MPP).
Figure 10: P-V curve of a solar cell in Perturb and Observe method
Figure 11: P-V curve of a solar cell in Perturb and Observe method
11
4.2.2 Incremental Conductance method
This method uses the PV array's incremental conductance ݀ܲ/ܸ݀ to compute the sign
of ݀ܲ/ܸ݀. When ݀ܲ/ܸ݀ is equal and opposite to the value of I/V (where ݀ܲ/ܸ݀ =0)
the algorithm knows that the maximum power point is reached and thus it terminates
and returns the corresponding value of operating voltage for MPP. This method tracks
rapidly changing irradiation conditions more accurately than P&O method. One
complexity in this method is that it requires many sensors to operate and hence is
economically less effective [5] and [6].
P=V*I
Differentiating w.r.t voltage yields;
12
Figure 12: P-V curve of a solar cell in Perturb and Observe method
4.2.3 Parasitic Capacitance method
This method is an improved version of the incremental conductance method, with the
improvement being that the effect of the PV cell's parasitic union capacitance is
included into the voltage calculation [5] and [6].
4.2.4 Constant Voltage method
This method which is a not so widely used method because of the losses during
operation is dependent on the relation between the open circuit voltage and the
maximum power point voltage. The ratio of these two voltages is generally constant
for a solar cell, roughly around 0.76. Thus the open circuit voltage is obtained
experimentally and the operating voltage is adjusted to 76% of this value [8].
4.2.5 Constant Current method
Similar to the constant voltage method, this method is dependent on the relation
between the open circuit current and the maximum power point current. The ratio of
13
these two currents is generally constant for a solar cell, roughly around 0.95. Thus the
short circuit current is obtained experimentally and the operating current is adjusted to
95% of this value [8].
The methods have certain advantages and certain disadvantages. Choice is to be made
regarding which algorithm to be utilized looking at the need of the algorithm and the
operating conditions. For example, if the required algorithm is to be simple and not
much effort is given on the reduction of the voltage ripple then P&O is suitable. But if
the algorithm is to give a definite operating point and the voltage fluctuation near the
MPP is to be reduced then the IC method is suitable, but this would make the
operation complex and more costly.
4.3 FLOW CHART OF MPPT ALGORITHMS
Two of the most widely used methods for maximum power point racking are studied
here. The methods are
1. Perturb & Observe Method.
2. Incremental Conductance Method.
The flow charts for the two methods are shown below.
14
Figure 13: Flow chart for perturb & observe
15
Figure 14: Flow chart of incremental conductance method
16
CONCLUSION & FUTURE WORK
5.1 CONCLUSION
In this report a detailed analysis of various maximum power point tracking algorithms
were carried out. Incremental Conductance algorithm which holds good performance
than any other methods under normal and varying atmospheric conditions. Power
output obtained from incremental conductance method is high us compared to other
methods under varying atmospheric conditions. Maximum Power Point Tracking
algorithm which place a major role for a grid connected Photo voltaic system. A most
suitable MPPT technique is chosen based on the implementation cost, number of
sensors required, complexity. So for residential and industrial purposes
INCREMENTAL CONDUCTANCE ALGORITHM performs better results.
17
REFERENCES
“A New VSAS approach for Maximum Power Tracking for Renewable Energy
Sources (RES)” Nacer K. M’Sirdi , Abdelhamid Rabhi , Mouna Abarkan
“PV Power System Using Maximum Power Point Tracking (Increment
Conductance Algorithm)” Vol. 3, Issue 5, May 2014 @IJIRSET, Mohammed
Ali Khalifa, Kamal Mohamed Saied,Sami Salem Bitro, Miftahul Anwar,
Muhammad Nizam
“New perturb and observe mppt algorithm and its validation using data from pv
module” @IJAET, Bikram Das ,Anindita Jamatia, Abanishwar Chakraborti
Prabir Rn.Kasari& Manik Bhowmik
“Analysis of Different MPPT Techniques” Vol. 5, Issue 3, March 2016
@IJAREEIE, Athira B,. Greeshma V,. Jeena Johnson
“A New Maximum Power Point Tracking for Photovoltaic Systems” Mohamed
Azab, International Journal of Electrical, Computer, Energetic, Electronic and
Communication Engineering Vol:2, No:8, 2008.
“Enhancement of Solar Photovoltaic Cell by Using Short-Circuit Current Mppt
Method” Burri Ankaiah, Jalakanuru Nageswararao @ www.ijesi.org
Volume 2 Issue 2 ǁ February. 2013 ǁ PP.45-50

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Seminar Report on MPPT

  • 1. i A SEMINAR REPORT ON MPPT Technology Submitted in partial fulfillment of the requirement of the award of the degree Of BACHELOR OF TECHNOLOGY IN Electronics and Communication Engineering Submitted To Submitted by Mr. Rohit Negi Manish Barthwal Mr. Ajay Kumar (142107) ECE-3rd year DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING G B PANT ENGINEERING COLLEGE PAURI GARHWAL (UTTARAKHAND) INDIA
  • 2. ii ACKNOWLEDGMENT I would like to thank respected Mr. Rohit Negi and Mr. Ajay Kumar for giving me such a wonderful opportunity to expand my knowledge for my own branch and giving me guidelines to present a seminar report. It helped me a lot to realize of what we study for. Secondly, I would like to thank my parents who patiently helped me as i went through my work and helped to modify and eliminate some of the irrelevant or un-necessary stuffs. Thirdly, I would like to thank my friends who helped me to make my work more organized and well-stacked till the end. Next, I would thank Microsoft for developing such a wonderful tool like MS Word. It helped my work a lot to remain error-free. Last but clearly not the least, I would thank The Almighty for giving me strength to complete my report on time.
  • 3. iii ABSTRACT Due to rapid growth in the semiconductor and power electronics techniques, PV energy is of increasing interest in electrical power applications. Photovoltaic (PV) energy is the most important energy resource since it is clean, pollution free, and inexhaustible It is important to operate PV energy conversion systems near the maximum power point to increase the output efficiency of PV arrays. The output power of PV arrays is always changing with weather conditions, i.e., solar irradiation and atmospheric temperature. Therefore, a MPPT control to extract maximum power from the PV arrays at real time becomes indispensable in PV generation system. In recent years, a large number of techniques have been proposed for tracking the maximum power point (MPP). Maximum power point tracking (MPPT) is used in photovoltaic (PV) systems to maximize the photovoltaic array output power, irrespective of the temperature and radiation conditions and of the load electrical characteristics the PV array output power is used to directly control the dc/dc converter, thus reducing the complexity of the system. The resulting system has high- efficiency; lower-cost this paper proposes a maximum-PowerPoint tracking (MPPT) method with a simple algorithm for photovoltaic (PV) power generation systems. The method is based on use of a Incremental conductance of the PV to determine an optimum operating current for the maximum output power. This work proposes on Investigation of Incremental conductance Based maximum Power Point Tracking for Photovoltaic System, to have the advantages of low frequency switching.
  • 4. iv TABLE OF CONTENTS ACKNOWLEDGEMENT ii ABSTRACT iii TABLE OF CONTENTS iv 1. INTRODUCTION 1 2. SOLAR CELL MODELING 2.1) MODELING OF SOLAR CELL 2 2.2) EFFECT OF IRRADIATION 4 2.3) EFFECT OF TEMPERATURE 5 3. BOOST CONVERTER 3.1) BOOST CONVERTER 7 3.2) MODES OF OPERATION 7 3.3) WAVEFORMS 8 4. MAXIMUM POWER POINT TRACKING 4.1) MAXIMUM POWER POINT TRACKING 9 4.2) METHODS OF MPPT 9 4.3) FLOW CHART OF ALGORITHMS 13 5. CONCLUSION & FUTURE WORK 5.1) CONCLUSION 16 5.2) FUTURE WORK 16 6. REFERENCE 17
  • 5. 1 INTRODUCTION One of the major concerns in the power sector is the day-to-day increasing power demand but the unavailability of enough resources to meet the power demand using the conventional energy sources. Demand has increased for renewable sources of energy to be utilized along with conventional systems to meet the energy demand. Renewable sources like wind energy and solar energy are the prime energy sources which are being utilized in this regard. The continuous use of fossil fuels has caused the fossil fuel deposit to be reduced and has drastically affected the environment depleting the biosphere and cumulatively adding to global warming. Solar energy is abundantly available that has made it possible to harvest it and utilize it properly. Solar energy can be a standalone generating unit or can be a grid connected generating unit depending on the availability of a grid nearby. Thus it can be used to power rural areas where the availability of grids is very low. Another advantage of using solar energy is the portable operation whenever wherever necessary. In order to tackle the present energy crisis one has to develop an efficient manner in which power has to be extracted from the incoming solar radiation. The power conversion mechanisms have been greatly reduced in size in the past few years. The development in power electronics and material science has helped engineers to come up very small but powerful systems to withstand the high power demand. But the disadvantage of these systems is the increased power density. Trend has set in for the use of multi-input converter units that can effectively handle the voltage fluctuations. But due to high production cost and the low efficiency of these systems they can hardly compete in the competitive markets as a prime power generation source. The constant increase in the development of the solar cells manufacturing technology would definitely make the use of these technologies possible on a wider basis than what the scenario is presently. The use of the newest power control mechanisms called the Maximum Power Point Tracking (MPPT) algorithms has led to the increase in the efficiency of operation of the solar modules and thus is effective in the field of utilization of renewable sources of energy.
  • 6. 2 SOLAR CELL MODELING 2.1 MODELLING OF SOLAR CELL A solar cell is the building block of a solar panel. A photovoltaic module is formed by connecting many solar cells in series and parallel. Considering only a single solar cell; it can be modeled by utilizing a current source, a diode and two resistors. This model is known as a single diode model of solar cell. Two diode models are also available but only single diode model is considered here [1], [2], [4], [7], [9] and [10]. Figure 2: Single diode model of a solar cell Fig.1: MPPT block scheme
  • 7. 3 The characteristic equation for a photovoltaic cell is given by [1], [2], [4], [7], [9] and [10], I & V : Cell output current and voltage; Ios : Cell reverse saturation current; T : Cell temperature in Celsius; k : Boltzmann's constant, 1.38 * 10-19 J/K; q : Electron charge, 1.6*10-23 C; Ki : Short circuit current temperature coefficient at Iscr; lambda : Solar irradiation in W/m^2; Iscr : Short circuit current at 25 degree Celsius; Ilg : Light-generated current; Ego : Band gap for silicon; A : Ideality factor; Tr : Reference temperature; Ior : Cell saturation current at Tr; Rsh : Shunt resistance; Rs : Series resistance; The characteristic equation of a solar module is dependent on the number of cells in parallel and number of cells in series. It is observed from experimental results that the current variation is less dependent on the shunt resistance and is more dependent on the series resistance [7].
  • 8. 4 The I-V and P-V curves for a solar cell are given in the following figure. It can be seen that the cell operates as a constant current source at low values of operating voltages and a constant voltage source at low values of operating current. Figure 3: P-V I-V curve of a solar cell at given temperature and solar irradiation 2.2 EFFECT OF VARIATION OF SOLAR IRRADIATION The P-V and I-V curves of a solar cell are highly dependent on the solar irradiation values. The solar irradiation as a result of the environmental changes keeps on fluctuating, but control mechanisms are available that can track this change and can alter the working of the solar cell to meet the required load demands. Higher is the solar irradiation, higher would be the solar input to the solar cell and hence power magnitude would increase for the same voltage value. With increase in the solar irradiation the open circuit voltage increases. This is due to the fact that, when more sunlight incidents on to the solar cell, the electrons are supplied with higher excitation energy, thereby increasing the electron mobility and thus more power is generated [7] and [10].
  • 9. 5 Figure 4: Variation of P-V curve with solar irradiation Figure 5: Variation of I-V curve with solar irradiation 2.3 EFFECT OF VARIATION OF TEMPERATURE On the contrary the temperature increase around the solar cell has a negative impact on the power generation capability. Increase in temperature is accompanied by a decrease in the open circuit voltage value. Increase in temperature causes increase in the band gap of the material and thus more energy is required to cross this barrier. Thus the efficiency of the solar cell is reduced [7] and [10].
  • 10. 6 Figure 6: Variation of P-V curve with temperature Figure 7: Variation of I-V with temperature
  • 11. 7 BOOST CONVERTER 3.1 BOOST CONVERTER Boost converter steps up the input voltage magnitude to a required output voltage magnitude without the use of a transformer. The main components of a boost converter are an inductor, a diode and a high frequency switch. These in a co- ordinated manner supply power to the load at a voltage greater than the input voltage magnitude. The control strategy lies in the manipulation of the duty cycle of the switch which causes the voltage change [11] and [12]. Figure 8: A boost converter 3.2 MODES OF OPERATION There are two modes of operation of a boost converter. Those are based on the closing and opening of the switch. The first mode is when the switch is closed; this is known as the charging mode of operation. The second mode is when the switch is open; this is known as the discharging mode of operation [12]. 3.2.1 Charging Mode In this mode of operation; the switch is closed and the inductor is charged by the source through the switch. The charging current is exponential in nature but for simplicity is assumed to be linearly varying [11]. The diode restricts the flow of
  • 12. 8 current from the source to the load and the demand of the load is met by the discharging of the capacitor. 3.2.2Discharging Mode In this mode of operation; the switch is open and the diode is forward biased [11]. The inductor now discharges and together with the source charges the capacitor and meets the load demands. The load current variation is very small and in many cases is assumed constant throughout the operation. 3.3 WAVEFORMS Figure 9: Waveforms of boost converter
  • 13. 9 MAXIMUM POWER POINT TRACKING 4.1 MAXIMUM POWER POINT TRACKING The efficiency of a solar cell is very low. In order to increase the efficiency, methods are to be undertaken to match the source and load properly. One such method is the Maximum Power Point Tracking (MPPT). This is a technique used to obtain the maximum possible power from a varying source. In photovoltaic systems the I-V curve is non-linear, thereby making it difficult to be used to power a certain load. This is done by utilizing a boost converter whose duty cycle is varied by using a mppt algorithm. Few of the many algorithms are listed below [3], [4], [5] and [8]. A boost converter is used on the load side and a solar panel is used to power this converter. 4.2 METHODS FOR MPPT There are many methods used for maximum power point tracking a few are listed below: • Perturb and Observe method • Incremental Conductance method • Parasitic Capacitance method • Constant Voltage method • Constant Current method 4.2.1 Perturb and Observe method This method is the most common. In this method very less number of sensors are utilized [5] and [6]. The operating voltage is sampled and the algorithm changes the operating voltage in the required direction and samples ݀ܲ/ܸ݀. If ݀ܲ/ܸ݀ is positive, then the algorithm increases the voltage value towards the MPP until ݀ܲ/ܸ݀ is negative. This iteration is continued until the algorithm finally reaches the MPP. This
  • 14. 10 algorithm is not suitable when the variation in the solar irradiation is high. The voltage never actually reaches an exact value but perturbs around the maximum power point (MPP). Figure 10: P-V curve of a solar cell in Perturb and Observe method Figure 11: P-V curve of a solar cell in Perturb and Observe method
  • 15. 11 4.2.2 Incremental Conductance method This method uses the PV array's incremental conductance ݀ܲ/ܸ݀ to compute the sign of ݀ܲ/ܸ݀. When ݀ܲ/ܸ݀ is equal and opposite to the value of I/V (where ݀ܲ/ܸ݀ =0) the algorithm knows that the maximum power point is reached and thus it terminates and returns the corresponding value of operating voltage for MPP. This method tracks rapidly changing irradiation conditions more accurately than P&O method. One complexity in this method is that it requires many sensors to operate and hence is economically less effective [5] and [6]. P=V*I Differentiating w.r.t voltage yields;
  • 16. 12 Figure 12: P-V curve of a solar cell in Perturb and Observe method 4.2.3 Parasitic Capacitance method This method is an improved version of the incremental conductance method, with the improvement being that the effect of the PV cell's parasitic union capacitance is included into the voltage calculation [5] and [6]. 4.2.4 Constant Voltage method This method which is a not so widely used method because of the losses during operation is dependent on the relation between the open circuit voltage and the maximum power point voltage. The ratio of these two voltages is generally constant for a solar cell, roughly around 0.76. Thus the open circuit voltage is obtained experimentally and the operating voltage is adjusted to 76% of this value [8]. 4.2.5 Constant Current method Similar to the constant voltage method, this method is dependent on the relation between the open circuit current and the maximum power point current. The ratio of
  • 17. 13 these two currents is generally constant for a solar cell, roughly around 0.95. Thus the short circuit current is obtained experimentally and the operating current is adjusted to 95% of this value [8]. The methods have certain advantages and certain disadvantages. Choice is to be made regarding which algorithm to be utilized looking at the need of the algorithm and the operating conditions. For example, if the required algorithm is to be simple and not much effort is given on the reduction of the voltage ripple then P&O is suitable. But if the algorithm is to give a definite operating point and the voltage fluctuation near the MPP is to be reduced then the IC method is suitable, but this would make the operation complex and more costly. 4.3 FLOW CHART OF MPPT ALGORITHMS Two of the most widely used methods for maximum power point racking are studied here. The methods are 1. Perturb & Observe Method. 2. Incremental Conductance Method. The flow charts for the two methods are shown below.
  • 18. 14 Figure 13: Flow chart for perturb & observe
  • 19. 15 Figure 14: Flow chart of incremental conductance method
  • 20. 16 CONCLUSION & FUTURE WORK 5.1 CONCLUSION In this report a detailed analysis of various maximum power point tracking algorithms were carried out. Incremental Conductance algorithm which holds good performance than any other methods under normal and varying atmospheric conditions. Power output obtained from incremental conductance method is high us compared to other methods under varying atmospheric conditions. Maximum Power Point Tracking algorithm which place a major role for a grid connected Photo voltaic system. A most suitable MPPT technique is chosen based on the implementation cost, number of sensors required, complexity. So for residential and industrial purposes INCREMENTAL CONDUCTANCE ALGORITHM performs better results.
  • 21. 17 REFERENCES “A New VSAS approach for Maximum Power Tracking for Renewable Energy Sources (RES)” Nacer K. M’Sirdi , Abdelhamid Rabhi , Mouna Abarkan “PV Power System Using Maximum Power Point Tracking (Increment Conductance Algorithm)” Vol. 3, Issue 5, May 2014 @IJIRSET, Mohammed Ali Khalifa, Kamal Mohamed Saied,Sami Salem Bitro, Miftahul Anwar, Muhammad Nizam “New perturb and observe mppt algorithm and its validation using data from pv module” @IJAET, Bikram Das ,Anindita Jamatia, Abanishwar Chakraborti Prabir Rn.Kasari& Manik Bhowmik “Analysis of Different MPPT Techniques” Vol. 5, Issue 3, March 2016 @IJAREEIE, Athira B,. Greeshma V,. Jeena Johnson “A New Maximum Power Point Tracking for Photovoltaic Systems” Mohamed Azab, International Journal of Electrical, Computer, Energetic, Electronic and Communication Engineering Vol:2, No:8, 2008. “Enhancement of Solar Photovoltaic Cell by Using Short-Circuit Current Mppt Method” Burri Ankaiah, Jalakanuru Nageswararao @ www.ijesi.org Volume 2 Issue 2 ǁ February. 2013 ǁ PP.45-50