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International Journal of Modern Engineering Research (IJMER)
               www.ijmer.com             Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671      ISSN: 2249-6645

                          Simulink Based Model of Photovoltaic Cell
                            *Mr. G. Venkateswarlu, **Dr.Psangameswar Raju
                                     *Prof in dept of EEE, Narayana Engg College, Nellore
                                              **Professor, S.V.Univesity, Tirupati.


ABSTRACT: The potential           for solar energy as a           phenomena and mismatch in photovoltaic cells association
sustainable source of energy is well understood. With the         have become interesting, these models have been reviewed
ever increasing use of solar power the necessity of a model       to deal with the reverse characteristics, when solar cells are
is accentuated. The aim of this work is to study the              working in reverse bias. One of the first approaches
variation of PV module main characteristic parameters as          modifies the one diode model with the assumption that the
a function of shading, with a special attention to the            avalanche multiplication affects mainly the direct current.
relationship between output power lowering due to                 The mathematical model of the solar cell taking into
shading.                                                          account the effect of breakdown voltage is given by the
                                                                  equation.
Keywords: pvc, mppt, solarex

               I.       INTRODUCTION
India is endowed with vast solar energy potential. About          Where the multiplication factor M(V) denotes the effect of
5,000 trillion kWh per year energy is incident over India’s       the avalanche effect.[5,6] The expression of M(V) is:
land area with most parts receiving 4-7 kWh per sq. m per
day. [1]From an energy security perspective, solar is the
most secure of all sources, since it is abundantly available.
The objective of the National Solar Mission is to establish
India as a global leader in solar energy, by creating the         where Vb is the breakdown voltage in reverse bias and n is
policy conditions for its diffusion across the country as         the Miller constant. Figure 1 shows the electrical
quickly as possible. To create an enabling policy                 equivalent circuit including the effect of M(V) modelled by
framework for the deployment of 20,000 MW of solar                a controlled current source. Bishop[7] proposed an
power by 2022.[1]                                                 equation where the avalanche effect is expressed as a non-
                                                                  linear multiplication factor that affects the shunt resistance
                                                                  current term. The proposed model is given by Equation (3)
     II.       SOLAR INSOLATION IN INDIA
                                                                  and the corresponding equivalent circuit is shown in Figure
With about 300 clear sunny days in a year, India's
                                                                  2.
theoretical solar power reception, just on its land area, is
about 5 PWh.[1] The daily average solar energy incident
over India varies from 4 to 7 kWh/m2 with about 2,300–
3,200 sunshine hours per year[1]. This is far more than
current total energy consumption. For example, even
assuming 10% conversion efficiency for PV modules, it
will still be thousand times greater than the likely
electricity demand in India by the year 2015[1]                   where Vb is the breakdown voltage, a and n are constants.
                                                                  The additional term, E(V), is added to the leakage current
       III.     PHOTOVOLTAIC MODULES                              into the shunt resistance term modeled as a controlled
Solar cells consist of a p-n junction fabricated in a thin        current source:
wafer or layer of semiconductor.[2] In the dark, the I-V
output characteristic of a solar cell has an exponential
characteristic similar to that of a diode.[2] .PV module
represents the fundamental power conversion unit of a PV
generator system. The output characteristics of PV module           V.       SIMULINK BASED MODEL FOR PV
depends on the solar insolation, the temperature and output                         MODULE
voltage of PV module.[2] Since PV module has nonlinear            The mathematical PV models used in computer simulation
characteristics, it is necessary to model it for the design and   have been built for over the pass four decades [6]-[8].
simulation of maximum power point tracking (MPPT) for             Almost all well-developed PV models describe the output
PV system applications.                                           characteristics mainly affected by the solar insolation, cell
                                                                  temperature, and load voltage. Most of the above models
     IV.       PHOTOVOLTAIC SOLAR CELL                            do not take into account the effects of shading on the PV
              MODELS IN REVERSE BIAS                              characteristics.
In order to describe the electrical behavior of a solar cell, in
light and darkness, the one diode model and the two diodes         We have chosen the Matlab/Simulink[12]environment to
model, derived from physical characteristics of solar cells,       study the effects of shadowing in PV module performance
are commonly used.[2] When investigations on hot spot              because Matlab is today a universal tool for mathematical
                                                         www.ijmer.com                                           2668 | Page
International Journal of Modern Engineering Research (IJMER)
               www.ijmer.com             Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671      ISSN: 2249-6645
applications and has been used before in PV systems’             power losses increase with increase of irradiation and
simulation and solar cell parameters’ extraction with            shadow rate.
success.[13,14]
The I–V characteristic simulation, in Matlab/ Simulink                          VI.      CONCLUSION
environment, of a photovoltaic module under different            An attempt has been made to model a photo voltaic cell
shadow rates was carried out using Bishop’s model                under the influence of shadow. The proposed model is
described in the previous section. The Solarex MSX60 PV          found be showing appreciable results in comparison with
[Table 1]module under study is formed by 36 serially             the data being supplied by the manufacturer It can also be
connected solar cells and one of the solar cells is assumed      applied to study the reverse characteristics of shadowed
to be shaded with variable rate of shadow: α (0≤ α ≤1) We        solar cells forming part of the PV module. The reduction in
consider that a full shadow corresponds to α =0 whereas α        the output power of a PV module due to shadowing has
=1 indicates no shadow present on the solar cell. The PV         been evaluated taking into account the influence of
module output voltage is the sum of voltages generated           irradiance level and the shadow rate over a cell of the PV
across the individual cells, illuminated and shaded:             module.




where Vis the total PV module voltage, and Vill_cell and
Vsh_cell are the voltages across the illuminated cells and
the shaded one, respectively. The current through all the
cells is the same:



where I is the current through the PV module, Iill_cell and        Figure 1: Solar cell equivalent circuit considering the
Ish_cell are the currents through the illuminated cells and                           avalanche effect
the shaded one, respectively.The following expression,
obtained from Equation (3) for the simulation of the I–V
characteristic of the PV module has been used:[3]




The same equation is governing the shaded cell with the
assumption that the photogenerated current is proportional
to the rate of shadow denoted by a. Thus the expression of
                                                                            Figure 2: Bishop’s equivalent circuit
the photogenerated current at the shaded cell is given by[7]



where ФN and Ф are the standard and incident irradiance,
respectively.
The output power of the whole PV module is always less
than the sum of the values of the individual power cells due
to dispersion of the parameters. These losses are
accentuated in the case of partial or full shadow of one or
several cells serially connected to form the PV module. We
have tried to report the amount of power lowering due to
shadow effect. The power loss is given by the following
expression



                                                                 Figure 3: A part of Simulink block used in simulation
where Pmax_unsh and Pmax_sh, are respectively the
maximum powers corresponding to the unshaded cells of
the PV module and the shaded one. A single solar cell
totally shaded does not cause a significant maximum power
loss; it is less than 10% at lower irradiation. Therefore, the
                                                       www.ijmer.com                                            2669 | Page
International Journal of Modern Engineering Research (IJMER)
              www.ijmer.com             Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671      ISSN: 2249-6645




                                                                Figure 7 :I-V characteristics of the photovoltaic cell under
                                                                                    different isolation
  Figure 4: NW India Direct Normal Solar Irradiance
                Annual Average [16]




                                                                Figure 8 :I–V characteristics of the photovoltaic cell under
 Figure 4: Monthly mean irradiance for Hyderabad[16]                                     shadow




                                                                        Table 1; Specifications of solarex MSX 60

Figure 6 :P-V characteristics of the photovoltaic cell under
                    different isolation




                                                      www.ijmer.com                                             2670 | Page
International Journal of Modern Engineering Research (IJMER)
             www.ijmer.com            Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671      ISSN: 2249-6645
                   REFERENCES
[1]   Jawaharlal Nehru National Solar Mission                 [9]    Kawamura H, Naka K, Yonekura N, Yamanaka
      Document                                                       S,Kawamura H, Ohno H, Naito K. Simulation of I-
[2]   S. W. Angrist, , Direct Energy Conversion, Allyn               Vcharacteristics of a PV module with shaded PV
      and Bacon, Inc., 4th edition, 1982, pp. 177-227.               cells.Solar energy Materials & Solar cells 2003; 75:
[3]   O. Wasynczuk, ―Dynamic behavior of a class of                  613–621.
      photovoltaic power systems,‖ IEEE Transactions on       [10]   Hermann W, Wiesner W. Modelling of PV
      Power Apparatus and Systems, vol. PAS-102, no. 9,              modules— the effects of non-uniform irradiance on
      1983, pp. 3031-3037.                                           performancemeasurements with solar simulators.
[4]   J. C. H. Phang, D. S. H. Chan, and J. R. Philips,              Proceedings of the 16th European Photovoltaic
      ―Accurate analytical method for the extraction of              Solar Energy Conference, 2000; 2338–234
      solar cell model parameters,‖ Electronics Letters,      [11]   Alonso Garcıa MC, Ruıエz JM. Analysis and
      vol. 20, no. 10, 1995.                                         modeling the reverse characteristic of photovoltaic
[5]   Spirito P, Abergamo V. Reverse bias power                      cells. Solar Energy Materials and Solar Cells 2006;
      dissipation of shadowed or faulty cells in different           90: 1105–1120.
      array configurations. Proceedings of the Fourth         [12]    http://www.mathworks.com/
      European Photovoltaic Solar Energy Conference,          [13]   Silvestre S, Guasch D, Ortega P, Calatayud R.
      1982; 296–300.                                                 Photovoltaic systems modelling using matlab and
[6]   Lopez Pineda CF. Experimental evaluation of                    simulink.
      reverse bias stress induced on photovoltaic modules            Proceedings of the 19th European Photovoltaic
      for different configurations. Solid Wind Technology            Solar Energy Conference, 2004; 2207–2210.
      1986; 3(2): 85–88.                                      [14]   Ortega P, Silvestre S, Guasch D, Navarro D,
[7]   Bishop JW. Computer simulation of the effects of               Calatayud R. Solar cell model parameter extractor
      electrical mismatches in photovoltaic cell                     based on matlab.
      interconnection circuits. Solar Cells 1998; 25: 73–            Proceedings of the 19th European Photovoltaic
      89.                                                            Solar Energy Conference, 2004; 2194–2197.
[8]   Quaschning V, Hanitsch R. Numerical simulation of       [15]   Meyer EL, Van Dyk EE. The effect of reduced
      photovoltaic generators with shaded cells.                     Shunt Resistance and shading on photovoltaic
      Proceedings Of the 30th Universities Power                     module performance. Proceedings of the 31 IEEE
      Engineering Conference,1995; 583–586.                          Photovoltaic Specialists Conference, 2005; 1331–
                                                                     1334. Copyright
                                                              [16]   Solar radiation Handbook 2008




                                                    www.ijmer.com                                            2671 | Page

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Ef2426682671

  • 1. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671 ISSN: 2249-6645 Simulink Based Model of Photovoltaic Cell *Mr. G. Venkateswarlu, **Dr.Psangameswar Raju *Prof in dept of EEE, Narayana Engg College, Nellore **Professor, S.V.Univesity, Tirupati. ABSTRACT: The potential for solar energy as a phenomena and mismatch in photovoltaic cells association sustainable source of energy is well understood. With the have become interesting, these models have been reviewed ever increasing use of solar power the necessity of a model to deal with the reverse characteristics, when solar cells are is accentuated. The aim of this work is to study the working in reverse bias. One of the first approaches variation of PV module main characteristic parameters as modifies the one diode model with the assumption that the a function of shading, with a special attention to the avalanche multiplication affects mainly the direct current. relationship between output power lowering due to The mathematical model of the solar cell taking into shading. account the effect of breakdown voltage is given by the equation. Keywords: pvc, mppt, solarex I. INTRODUCTION India is endowed with vast solar energy potential. About Where the multiplication factor M(V) denotes the effect of 5,000 trillion kWh per year energy is incident over India’s the avalanche effect.[5,6] The expression of M(V) is: land area with most parts receiving 4-7 kWh per sq. m per day. [1]From an energy security perspective, solar is the most secure of all sources, since it is abundantly available. The objective of the National Solar Mission is to establish India as a global leader in solar energy, by creating the where Vb is the breakdown voltage in reverse bias and n is policy conditions for its diffusion across the country as the Miller constant. Figure 1 shows the electrical quickly as possible. To create an enabling policy equivalent circuit including the effect of M(V) modelled by framework for the deployment of 20,000 MW of solar a controlled current source. Bishop[7] proposed an power by 2022.[1] equation where the avalanche effect is expressed as a non- linear multiplication factor that affects the shunt resistance current term. The proposed model is given by Equation (3) II. SOLAR INSOLATION IN INDIA and the corresponding equivalent circuit is shown in Figure With about 300 clear sunny days in a year, India's 2. theoretical solar power reception, just on its land area, is about 5 PWh.[1] The daily average solar energy incident over India varies from 4 to 7 kWh/m2 with about 2,300– 3,200 sunshine hours per year[1]. This is far more than current total energy consumption. For example, even assuming 10% conversion efficiency for PV modules, it will still be thousand times greater than the likely electricity demand in India by the year 2015[1] where Vb is the breakdown voltage, a and n are constants. The additional term, E(V), is added to the leakage current III. PHOTOVOLTAIC MODULES into the shunt resistance term modeled as a controlled Solar cells consist of a p-n junction fabricated in a thin current source: wafer or layer of semiconductor.[2] In the dark, the I-V output characteristic of a solar cell has an exponential characteristic similar to that of a diode.[2] .PV module represents the fundamental power conversion unit of a PV generator system. The output characteristics of PV module V. SIMULINK BASED MODEL FOR PV depends on the solar insolation, the temperature and output MODULE voltage of PV module.[2] Since PV module has nonlinear The mathematical PV models used in computer simulation characteristics, it is necessary to model it for the design and have been built for over the pass four decades [6]-[8]. simulation of maximum power point tracking (MPPT) for Almost all well-developed PV models describe the output PV system applications. characteristics mainly affected by the solar insolation, cell temperature, and load voltage. Most of the above models IV. PHOTOVOLTAIC SOLAR CELL do not take into account the effects of shading on the PV MODELS IN REVERSE BIAS characteristics. In order to describe the electrical behavior of a solar cell, in light and darkness, the one diode model and the two diodes We have chosen the Matlab/Simulink[12]environment to model, derived from physical characteristics of solar cells, study the effects of shadowing in PV module performance are commonly used.[2] When investigations on hot spot because Matlab is today a universal tool for mathematical www.ijmer.com 2668 | Page
  • 2. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671 ISSN: 2249-6645 applications and has been used before in PV systems’ power losses increase with increase of irradiation and simulation and solar cell parameters’ extraction with shadow rate. success.[13,14] The I–V characteristic simulation, in Matlab/ Simulink VI. CONCLUSION environment, of a photovoltaic module under different An attempt has been made to model a photo voltaic cell shadow rates was carried out using Bishop’s model under the influence of shadow. The proposed model is described in the previous section. The Solarex MSX60 PV found be showing appreciable results in comparison with [Table 1]module under study is formed by 36 serially the data being supplied by the manufacturer It can also be connected solar cells and one of the solar cells is assumed applied to study the reverse characteristics of shadowed to be shaded with variable rate of shadow: α (0≤ α ≤1) We solar cells forming part of the PV module. The reduction in consider that a full shadow corresponds to α =0 whereas α the output power of a PV module due to shadowing has =1 indicates no shadow present on the solar cell. The PV been evaluated taking into account the influence of module output voltage is the sum of voltages generated irradiance level and the shadow rate over a cell of the PV across the individual cells, illuminated and shaded: module. where Vis the total PV module voltage, and Vill_cell and Vsh_cell are the voltages across the illuminated cells and the shaded one, respectively. The current through all the cells is the same: where I is the current through the PV module, Iill_cell and Figure 1: Solar cell equivalent circuit considering the Ish_cell are the currents through the illuminated cells and avalanche effect the shaded one, respectively.The following expression, obtained from Equation (3) for the simulation of the I–V characteristic of the PV module has been used:[3] The same equation is governing the shaded cell with the assumption that the photogenerated current is proportional to the rate of shadow denoted by a. Thus the expression of Figure 2: Bishop’s equivalent circuit the photogenerated current at the shaded cell is given by[7] where ФN and Ф are the standard and incident irradiance, respectively. The output power of the whole PV module is always less than the sum of the values of the individual power cells due to dispersion of the parameters. These losses are accentuated in the case of partial or full shadow of one or several cells serially connected to form the PV module. We have tried to report the amount of power lowering due to shadow effect. The power loss is given by the following expression Figure 3: A part of Simulink block used in simulation where Pmax_unsh and Pmax_sh, are respectively the maximum powers corresponding to the unshaded cells of the PV module and the shaded one. A single solar cell totally shaded does not cause a significant maximum power loss; it is less than 10% at lower irradiation. Therefore, the www.ijmer.com 2669 | Page
  • 3. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671 ISSN: 2249-6645 Figure 7 :I-V characteristics of the photovoltaic cell under different isolation Figure 4: NW India Direct Normal Solar Irradiance Annual Average [16] Figure 8 :I–V characteristics of the photovoltaic cell under Figure 4: Monthly mean irradiance for Hyderabad[16] shadow Table 1; Specifications of solarex MSX 60 Figure 6 :P-V characteristics of the photovoltaic cell under different isolation www.ijmer.com 2670 | Page
  • 4. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug. 2012 pp-2668-2671 ISSN: 2249-6645 REFERENCES [1] Jawaharlal Nehru National Solar Mission [9] Kawamura H, Naka K, Yonekura N, Yamanaka Document S,Kawamura H, Ohno H, Naito K. Simulation of I- [2] S. W. Angrist, , Direct Energy Conversion, Allyn Vcharacteristics of a PV module with shaded PV and Bacon, Inc., 4th edition, 1982, pp. 177-227. cells.Solar energy Materials & Solar cells 2003; 75: [3] O. Wasynczuk, ―Dynamic behavior of a class of 613–621. photovoltaic power systems,‖ IEEE Transactions on [10] Hermann W, Wiesner W. Modelling of PV Power Apparatus and Systems, vol. PAS-102, no. 9, modules— the effects of non-uniform irradiance on 1983, pp. 3031-3037. performancemeasurements with solar simulators. [4] J. C. H. Phang, D. S. H. Chan, and J. R. Philips, Proceedings of the 16th European Photovoltaic ―Accurate analytical method for the extraction of Solar Energy Conference, 2000; 2338–234 solar cell model parameters,‖ Electronics Letters, [11] Alonso Garcıa MC, Ruıエz JM. Analysis and vol. 20, no. 10, 1995. modeling the reverse characteristic of photovoltaic [5] Spirito P, Abergamo V. Reverse bias power cells. Solar Energy Materials and Solar Cells 2006; dissipation of shadowed or faulty cells in different 90: 1105–1120. array configurations. Proceedings of the Fourth [12] http://www.mathworks.com/ European Photovoltaic Solar Energy Conference, [13] Silvestre S, Guasch D, Ortega P, Calatayud R. 1982; 296–300. Photovoltaic systems modelling using matlab and [6] Lopez Pineda CF. Experimental evaluation of simulink. reverse bias stress induced on photovoltaic modules Proceedings of the 19th European Photovoltaic for different configurations. Solid Wind Technology Solar Energy Conference, 2004; 2207–2210. 1986; 3(2): 85–88. [14] Ortega P, Silvestre S, Guasch D, Navarro D, [7] Bishop JW. Computer simulation of the effects of Calatayud R. Solar cell model parameter extractor electrical mismatches in photovoltaic cell based on matlab. interconnection circuits. Solar Cells 1998; 25: 73– Proceedings of the 19th European Photovoltaic 89. Solar Energy Conference, 2004; 2194–2197. [8] Quaschning V, Hanitsch R. Numerical simulation of [15] Meyer EL, Van Dyk EE. The effect of reduced photovoltaic generators with shaded cells. Shunt Resistance and shading on photovoltaic Proceedings Of the 30th Universities Power module performance. Proceedings of the 31 IEEE Engineering Conference,1995; 583–586. Photovoltaic Specialists Conference, 2005; 1331– 1334. Copyright [16] Solar radiation Handbook 2008 www.ijmer.com 2671 | Page