 Open Access
 Total Downloads : 98
 Authors : M. Vinay Kumar , U. Salma
 Paper ID : IJERTV6IS120146
 Volume & Issue : Volume 06, Issue 12 (December 2017)
 DOI : http://dx.doi.org/10.17577/IJERTV6IS120146
 Published (First Online): 26122017
 ISSN (Online) : 22780181
 Publisher Name : IJERT
 License: This work is licensed under a Creative Commons Attribution 4.0 International License
Mathematical Modeling of a Solar Cell and its Performance Analysis under Uniform and NonUniform Insolation
M. Vinay Kumar
Department of Electrical & Electronics Engineering, GMR Institute of Technology, Rajam
U. Salma
Department of Electrical & Electronics Engineering, Git
Gitam University, Visakapatnam
Abstract – Solar photovoltaic (PV)based electric power generation is gainingmuch importance due to huge availability of solar energy, developments inPV cell materials and energy transformation technology. Global warming effects and fast depletion of fossil fuelsis directly encouraging thistransformation process.The electric power produced by solar PV module depends on theinsolation and temperature.This paper presents a mathematicalmodel for a solar photovoltaic PVcell in order to evaluate its electrical characteristics with respect to weather conditions such as uniform insolation, change in insolationand change in temperature. The solar PV cell is modeledthrough mathematical equations and is representedby an equivalent circuit having a photocurrent source, a diode, a series resistor and a shunt resistor. As the performance of a solar PV array getsaffected by PV array insolation and temperature, it isimportant to understand the relation between these effects and its dependence on the output electric power of PV array. The main purpose of this paper is to consider the effects of sunlight insolation and celltemperature, then output current and voltage (IV) characteristics, output powerand voltage (PV) characteristics of PV model are simulated with help of Matlab simulation. This model is designed with a userfriendly icon and adialog box like Simulink block libraries and it has beendeveloped using Matlab/Simulinksoftware package.
Keywords – Solar Cell Model, Solar Array Model, Solar Insolation, Maximum Power Point Tracker, Matlab, SIMULINK

INTRODUCTION
With increasing alarms about skyrocketing oil prices, depletion of fossil fuel, global warming and destruction to environment and ecosystem, the alternative solution for the above mentioned concerns is to be overcome, the only solution is theusage of alternative energy resources with high efficiency and low emission of gases.
The alternative energy resources are renewable energy sources are also called asnonconventional energy sources,these arecontinuously renewed by natural biological process. These include solarenergy, wind energy, ocean energy, tidal energy,geo thermal energy, hydropower,bioenergy – bio fuelsetc., are few examples ofrenewable energy sources. A renewable energy system transformsthe energy found in sunlight, wind, seawaves, fallingwater, geothermal heat, or biomass into required forms, such as in the form of electrical energy or heat energy.
In spite of the intermittency of sunlight, solar energy is broadly available and it is completely free of cost. A photovoltaic (PV) system converts solar energy into electrical
energy. PV system is generally utilized in the forefront for electric power generation. It can generate direct current electricity without environmental pollution when exposed to solar radiation. PV systems are gaining more attention as renewable energy source as it does not pollute, has no fuel cost, doesnt contain any moving parts, hence no operating noise, requires less maintenance costs.etc.,
The basic element of a PV system is a PV cell. A PV array consists of several cells connected in series and/or parallelfor having a higher current/ voltage rating of the PV array.
Fig.1.Photovoltaic cell, module, panels and arrays
Model for a PV cell or a PV module based on the Shockley diode equation is presented [1], [2]. PV system sometimes may operate in conditions which results in non uniform irradiance of PV arrays due to bird dropping, debris, dust, leaves, clouds, shadows etc., if number of PV cells are mismatched due to nonuniform irradiance, such cells will limit the output current of normal PV cells [7][10]. These operating conditions leads to reduction in output power, generation of hot spot and finally causes damage to the cell. To protect the PV cells a bypass diode is connected in parallel. To obtain maximum output from a PV system, it is very important to have the knowledge of PV cell characteristics under non uniform irradiance [11][13].
The productivity of a PV array system depends on the working conditions. The current, output voltage and power of PV array fluctuate according to solarirradiation level, temperature and load current.These PV systems used as distributed generators (DG) and canbe located at the places where the demand of electric energy ascends,therebyavoiding
losses of transmission and also contributing in reductions tothe CO2 emission.This paper presents MatlabSimulink based PV module model, which can be seriesparalleled to achieve require currentvoltage rating of PV array.
.

PHOTOVOLTAIC MODELING
An ideal PV cell is modeled with a current source connected diode in antiparallel.For a nonideal PV cell, series resistance and a shunt resistance are connected. The value of series resistance is very small and that of a shunt resistance is very large.PV systemdisplays a nonlinear IV and PV
Voc : open circuit voltage Vt : thermal voltage
RSe: series resistance RSh: shunt resistance
NSe: number of cells in series NSh: number of cells in parallel Sr:solar reference irradiation S:solar cell operating irradiation a: ideality factor
The mathematical equations of asolar cell are given below. Using Kirchoffs first law
characteristicswhich fluctuate with the radiant intensity and
I PV
I Ph Id I sh
operating cell temperature.
(1)
S

Mathematical model of aPhotovoltaic Cell
I Ph I scr Ki T Tr
S
r
VPV I PV RSe
d o aV
Solar PV cell is a basic component of a PV system,it comprises
of ptype and ntype semiconductors and ismanufactured as a pn junction on a thin wafer of semiconductor. The output of
I I exp 1
t
T 3 qE
Io Irs
exp go
T
Tr
1 1
each PV cell is around 0.5V to 0.7V. When theyare connected
in series,net output voltage increasesand when connected in
Tr
I
Irs scr
parallel,net output currentincreases.
exp qVoc
1
There are many equivalent circuits for a PV cell, a
AKT
VPV I PV RSe
single diode, a two diode model are mostly used. A single
diode model being simple and accurate is taken up in this
I sh
RSh
paper.The basic circuit of a single diode model for asolar PV
The load current Ipv is given as
V I R
V I R (2)
cell [3][6]is shown in Fig.2.
I PV I Ph Io exp PV
PV Se 1 PV
PV Se
Practical PV device
aVt
RSh
KT
Vt
IPV
Ideal PV cell
q
RSe
+
Photovoltaic cell characteristic curves, IV, PV curves are obtained by simulationequation (2).
ISh
Id

Mathematical model of a Photovoltaic Module
–
IPh
VPV
RSh
D
A number of Photovoltaic cells are connected in series parallel to form an array, number of such arrays are further connected toform panels or modules. The solar PV system converts irradiation is directly to electrical energy through photovoltaic effect. The Fig. 3 shows uniform insolation on a photovoltaic system.
IPV +
DBL DBL DBL
Fig.2. Equivalent circuit of a single solar cell
PV ARRAY
DBY
PV ARRAY
DBY
PV ARRAY
DBY
The symbols for the above circuit are as follows:
PV DBY PV
DBY PV
DBY
Iph: photo current
ARRAY
ARRAY
ARRAY
VPV
Ipv: output current Id : diode current Ish: shunt current
Io : reverse saturation current
Ior: reverse saturation current at reference temperature Iscr: short circuit current
PV ARRAY
PV ARRAY
DBY
DBY
PV ARRAY
PV ARRAY
DBY
DBY
PV ARRAY
PV ARRAY
DBY
DBY
–
Tr: reference temperature
T: cell operating temperature Ego : band gap energy
q :charge of a electron = 1.6 * 1019coloumbs
K :Boltzmans constant = 1.3805 * 1023 J/K
Ki : temperature coefficient of short cuit current Kv : temperature coefficient of open circuit voltage Vt : thermal voltage
VPV :output voltage
Fig.3. Uniform insolation for a photovoltaic system
The blocking diodes and bypass diodes are generally used in PV systems in series/parallel with PV arrays. A blocking diode allows flow of current from a PV panel to the battery for charging, ie., storing energy during day time, but does not allow the current to flow back from the battery to the PV panel during night times, hence preventing them from discharging.By pass diodes are connected in parallel with PV panels for a multi string PV panel
system. These bypasses the path of the current from the shaded panel and provides an alternate path for the current flow and hence maintaining continuity of power supply. Based on single PV cell circuit module, the voltage andcurrent relationship of a PV module can be represented as (3).


PV MODULE MODEL IN MATLABSIMULINK A 175W PV module BP 4175B has been chosen for modeling inMatlabSimulink environment. Theconcerned Electrical characteristics specifications are shown intableI.
VPV I PV RSe
Table.IElectrical characteristics
I N I
N N

N I exp Se Sh
PV Sh Ph
Sh o
aVt
1
VPV
N

I PV RSe N
Se Sh
RSh
(3)

Photovoltaic Cell/module under NonUniform insolation
Under uniform insolation, Eq. (3) is able to precisely model the performance of PV module. But for non uniform insolation, ie.,.under partial shading condition Eq. (3) cannot simulate this weather condition. The Fig. 4 shows non uniform insolation on a photovoltaic system. This non uniform insolation may occur due to various factors like bird droppings, passing of aeroplane, clouds,etc., The shaded PV arrays signify that solar insolation on them is less or nil as compared to the shaded PV array, hence their output power is either low or zero. To maintain the continuity of power production all the PV panels have bypass diode connected in parallel with PV panels, and in such case these types of panels are eliminated and the flow of current follows the bypass diode, hence maintaining continuous power production. The bypass diodes also prevents the flow of current from uniform insolated PV panel which are at higher potential to the less insolated or shaded PV panel which is at a lower potential. Hence, even under non uniform insolation condition the bypass diode helps in operating the whole solar PV system and produce electricity at a lower rate.
Parameter
Value
Maximum Power
400 W
Voltage at maximum power
32.5 V
Current at maximum power
13.94 A
Shortcircuit current
15.5 A
Opencircuit voltage
38.6 V
Temperature coefficient of opencircuit voltage
0.065 %/0C
Temperature coefficient of shortcircuit current
0.5 %/0C


SIMULATION RESULTS
This section presents the simulation resultsof the PV cell at different weather conditions like constant temperature at different insolations and constant insolation at different temperatures. Also the simulation results of the PV cell at non uniform insolation are presented.
A. Illustration I (uniform insolation)
For a single PV module, the IV, PV characteristics at uniform insolationsare presented below. The IV, PV curves at a constant temperature of 25 but at different insolation levels are shown in Fig. 5& Fig. 6 respectively. The solar insolationsare 1000W/m2, 800W/m2, 600W/m2, 400W/m2, and 200W/m2 respectively.
DBL DBL DBL
IPV +
PV ARRAY
PV ARRAY
PV ARRAY
PV ARRAY
DBY
DBY
DBY
DBY
PV ARRAY
PV ARRAY
PV ARRAY
PV ARRAY
DBY
DBY
DBY
DBY
PV ARRAY
PV ARRAY
PV ARRAY
PV ARRAY
DBY
DBY
DBY
DBY
VPV
Fig.5. IV Characteristics at constantFig. 6. PV Characteristics at constant temperature& various insolation levelstemperature &various insolation levels
The IV, PV curves at a constant insolation of 800 W/m2and at different temperatures are shown in Fig. 7& Fig. 8 respectively.The temperatures are 250C (2980 K), 350C (3080
K) and 450C (3180 K) respectively.
–
Fig.4. NonUniform insolation for a photovoltaic system
Asthe effects of nonuniform insolation on a solar module cannot be obtained from mathematical model ie., Eq. (3),the solarphoto current is used which is denoted by a current source and the effectscan be simulated by changing the values of current source.
Fig. 7. IV Characteristics at constant Fig. 8. PV Characteristics at constant insolation& various temperaturesinsolation & various temperatures
The IV, PV curves at nonunifrom insolation at two differentinsolation of 800 W/m2and 500 W/m2 at a constant temperature of 400C(3130 K) is shown in Fig. 9& Fig. 10 respectively
Fig.6.IV Characteristics of a Partial Fig. 6. PV Characteristics of a Partial shading PV system shading PV system

CONCLUSION
A PV module model simulation using MATLABSimulink software is presented in this paper. Using this model IV andP V characteristics can be studied with different weather conditions of insolation and temperature, i.e., under uniform and insolationnonuniform insolation. When PV modules are exposed tononuniform insolation, multiple peaks in IV, PV characteristics are formed. If the PV system has to operate at maximum efficiency, it needs to track the power at global peak and hence should be able to discriminate between local peak and global peak.
The conclusion drawn from the simulation results are as follows

During uniform insolation of a PV modules, there exists only one peak for each IV and PV characteristics

During nonuniform insolation of a PV modules, there exists multiple peaks for both IV and PV
characteristics

The number of power peaks are directly proportional to
number of insolation levels on PV modules, during nonuniform insolation of a PV modules.

During nonuniform insolation of a PV modules, the output power produced is more for the same series string.
The simulation not only just gives IV and PV characteristics, i.e., the behavior of PV array, but also its study helps in developing electronic circuit for maximum power point tracker for tracking maximum power from PV characteistics where the system needs to operate, hence new MPPT strategies can be developed. The presented results will help in designing best configuration of PV array to produce maximum output power.
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