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Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
Copyright © Faculty of Engineering, University of Maiduguri, Maiduguri, Nigeria.
Print ISSN: 1596-2490, Electronic ISSN: 2545-5818, www.azojete.com.ng
97
MPPT-BASED CONTROL ALGORITHM FOR PV SYSTEM USING ITERATION-
PSO UNDER IRREGULAR SHADOW CONDITIONS
M. Abdulkadir*, A. L. Bukar and B. Modu
(Department of Electrical and Electronics Engineering, Faculty of Engineering, University of
Maiduguri, Maiduguri, Nigeria)
*Corresponding author’s e-mail address: abdulkadirmusa@unimaid.edu.ng; Tel.: 08083831978
Co-authors e-mail address: abbalawan9@gmail.com, engrbb05@hotmail.com.
Abstract
The conventional maximum power point tracking (MPPT) techniques can hardly track the global maximum
power point (GMPP) because the power-voltage characteristics of photovoltaic (PV) exhibit multiple local
peaks in irregular shadow, and therefore easily fall into the local maximum power point. These conditions make
it very challenging, and to tackle this deficiency, an efficient Iteration Particle Swarm Optimization (IPSO) has
been developed to improve the quality of solution and convergence speed of the traditional PSO, so that it can
effectively track the GMPP under irregular shadow conditions. This proposed technique has such advantages as
simple structure, fast response and strong robustness, and convenient implementation. It is applied to MPPT
control of PV system in irregular shadow to solve the problem of multi-peak optimization in partial shadow. In
order to verify the rationality of the proposed algorithm, however, recently the dynamic MPPT performance
under varying irradiance conditions has been given utmost attention to the PV society. As the European standard
EN 50530 which defines the recommended varying irradiance profiles, was released lately, the corresponding
researchers have been required to improve the dynamic MPPT performance. This paper tried to evaluate the
dynamic MPPT performance using EN 50530 standard. The simulation results show that iterative-PSO method
can fast track the global MPP, increase tracking speed and higher dynamic MPPT efficiency under EN 50530
than the conventional PSO.
Keywords: Photovoltaic, iteration-PSO, MPPT, Controller, Irregular shadow, EN 50530
1. Introduction
In the past decade, the photovoltaic (PV) system has gained wide popularity as a renewable-
energy source due to depletion of conventional energy sources as well as the high cost of
conventional energy sources and their negative effects on the environment. An essential
feature of all PV systems is the efficacy of its maximum power point tracking (MPPT). This
technique has drawn immense attention from photovoltaic researchers and industry experts as
the most economical means to enhance the photovoltaic system efficiency. MPPT is
primarily an operating point co-coordinating the PV module and the DC-DC converter.
However, MPPT is not simple and easy to track because of the non-linear I–V characteristics
of the PV curve and the effect of partial shading causing the inconsistent in irradiance and
temperature. Therefore, tracking the accurate maximum power point (MPP) has been always
an intricate issue. The tracking eventually becomes sophisticated when all the PV modules do
not experience constant irradiance.
Several MPPT techniques have been proposed (Petreus et al., 2010; Ishaque et al., 2011; and
Abdulkadir et al., 2012). These methods differ in their accuracy, speed or complexity.
(Hossain et al. 2013; Eltawil et al, 2013; and David et al, 2014) reviewed and discussed
various techniques. For the partially-shaded condition where the shaded cell in a PV module
causes a decrease in power, the conventional MPPT technique becomes invalid due to the PV
characteristics becoming more complicated and also displaying multiple MPP. This effect of
partial shading has been analyzed by many researchers (La Manna et al., 2014 and Ishaque et
al., 2011). (Zegaoui et al, 2011) proposed a two-stage technique to track the global MPP. In
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
98
the first stage, the operating point of the PV system moves from the vicinity of the global
MPP by estimating the equivalent load line. Then, in the second stage, the incremental
conductance method is employed which converges the MPP. However, this method fails to
track the global MPP if the global MPP lies on the left of the load line. In (Miyatake et al.,
2011), a global stage was employed to locate the regions of the local MPP, while a perturb-
and-observe algorithm was employed at the local stage to find the global MPP. A sequential
extremum seeking control (ESC)-based MPPT technique was proposed in (Luo et al., 2009)
based on approximate modelling and analysis of the characteristics of PV modules under
variable partial-shading conditions. However, this method exhibits steady-state error and is
system-dependent. (Zang et al. 2012) proposed a PV system which adapts the parallel
configuration at a particular cell level so that an individual cell in the PV module can achieve
its MPP under partial-shading conditions. The input voltage of this configuration is very low,
which may increase the difficulty of designing an appropriate power converter. Moreover, the
proposed configuration is only suitable for low power applications.
Particle swarm optimization (PSO) has high potential for MPPT due to its simple structure,
easy implementation and fast computation capability. Since PSO is based on search
optimization in principle, it should be able to locate the MPP for any type of PV curve
regardless of environmental variations. The direct control structure was adopted by some
researchers for the PSO algorithm, where the positions of the PSO particles are used as the
duty cycles. Excellent dynamic tracking speeds under severe partial-shading conditions were
able to be handled using the method. Furthermore, the steady state oscillations were found to
be exceptionally low. For instance, to track the global point in a constant bus voltage
application, the conventional PSO was utilized in (Venugopalan et al., 2013). An analytical
expression of the objective functions based on PV current, irradiance and temperature was
formulated as in (Miyatake et al., 2011) and the conventional PSO was then utilized to track
the MPP.
The current-based PSO method was proposed by (Miyatake et al. 2011), where the series
inductor current of the boost converter is used as the reference signal to generate the pulse
width modulation signals for the switching converter. A repulsive term in the velocity
equation of the PSO was also introduced (Phimmasone et al., 2009). (Miyatake et al. 2011)
proposed an adaptive perceptive PSO (APPSO)-based MPPT algorithm. Ishaque et al.
presented an improved PSO-based MPPT algorithm for PV systems and discussed the
advantages of using PSO in conjunction with the direct duty cycle control in detail. However,
no system design guidelines and practical design considerations are provided in these papers.
(Miyatake et al. 2011) attempted to approach the global MPP using the PSO algorithm. In
these investigations, the authors tried to realize centralized MPPT control of the modular
(multi-module) PV system (Coelho et al, 2010). These MPPT algorithms have good
performance under various partial-shading conditions; however, these methods are only
suitable for systems that consist of multiple converters.
Therefore, the conventional maximum power point tracking (MPPT) techniques can hardly
track the global maximum power point (GMPP) because the power-voltage characteristics of
photovoltaic (PV) exhibit multiple local peaks in irregular shadow, and therefore easily fall
into the local maximum power point. These conditions make it very challenging, and to
tackle this deficiency, an efficient Iteration Particle Swarm Optimization (IPSO) has been
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
99
developed to improve the quality of solution and convergence speed of the traditional PSO
(Phimmasone et al., 2009, Liu and Liu, 2011), so that it can effectively track the GMPP
under irregular shadow conditions. This proposed technique has such advantages as simple
structure, fast response and strong robustness, and convenient implementation. It is applied to
MPPT control of PV system in irregular shadow to solve the problem of multi-peak
optimization in partial shadow. In order to verity the rationality of the proposed algorithm,
however, recently the dynamic MPPT performance under varying irradiance conditions has
been given utmost attention to the PV society. As the European standard EN 50530 which
defines the recommended varying irradiance profiles, was released lately, the corresponding
researchers have been required to improve the dynamic MPPT performance. This paper also
tries to evaluate the dynamic MPPT performance using EN 50530 standard. The simulation
results show that iterative-PSO method can fast track the global MPP, increase tracking speed
and higher dynamic MPPT efficiency under EN 50530 than the conventional PSO.
2. Materials and Methods
2.1 Particle Swam Optimization
PSO is a stochastic, population-based evolutionary algorithm search method, modelled after
the behavior of bird flocks (Miyatake et al., 2007). The PSO algorithm maintains a swarm of
individuals (called particles), where each particle represents a candidate solution. Particles
follow a simple behavior: they emulate the success of neighboring particles and their own
achieved success. The position of a particle is therefore influenced by the best particle (pbest)
in a neighborhood, as well as the best solution found by all the particles in the entire
population (gbest). The particle position, xi, is adjusted using:
(1)
where the velocity component, , represents the step size.
The velocity is calculated by:
( ) ( )
(2)
where denotes the particle position for i; the velocity of the particle at i is represented by
vi; the number of iterations is denoted by t; the inertia weight is represented by ω; and
are uniformly distributed random variables within [0, 1]; and the cognitive and social
coefficients are denoted by , respectively (Venugopalan et al., 2013, Chen et al, 2010).
The best position for the storage of the ith particle that has been found so far is denoted by
the variable pbest,i and the best position for the storage of all the particles is represented by
gbest. Figure 1 depicts the movement of the particle in the optimization process.
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
100
Figure 1: Movement of particles in the optimization process
2.2 Iterative Particle Swarm Optimization
A new PSO technique is introduced in this paper to mitigate the effect of oscillations in
maximum power point tracking power systems. The standard PSO is modified by adding a
new directory called Iterative Best (Ibest) to enhance the computational time and the quality of
the solution. Ibest is known to be the best value of the fitness function that will be achieved by
any agent (particle) in the iteration. A new PSO strategy time varying acceleration coefficient
is also introduced. Equation (7) shows the modified form of (3) and is referred to as the
Repetitive Particle Swarm Optimization (RPSO) here.
( ) ( ) ( )
(3)
where c3 represents the weight of the stochastic acceleration terms that is pulling each agent
towards the iteration best. refers to the best value of the fitness function that has been
obtained by any agent in the tth
iteration during optimization process. The cognitive and
social learning factors c1 and c2 in the classical PSO algorithm are usually pre-specified to
fixed values of 2.0 basically (Chatteijee et al, 2013, Fu and Tong 2010). This may lead to
premature convergence and may allow the particles to wander around the search space due to
relatively high values of coefficients. The cognitive and social learning factors c1 and c2 are
updated as in equations (4) and (5) Furthermore, the dynamic acceleration constant parameter
c3 is introduced and presented in equation (6).
( ) (4)
( ) (5)
( ) ( ( )
) (6)
where t is number of iterations. Therefore, the new velocity update of the proposed algorithm
can be updated as follows:
( t
t
cc if
i 


11
,1c ) ( ) ( t
t
cc if
i 


22
,2c ) (
( )1()(c
)(
13
2

tcct

 ) ( )) (7)
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
101
Figure 2 depicts the convergence behaviors for the IPSO algorithm fitness over the original
PSO, it can be seen that the fitness value of IPSO offers better result as compared to the
original PSO. Not only that, IPSO also convergence faster with attractive result (3rd
iteration)
compared to the PSO algorithm that required nearly 10th
iteration before it converged. Even
though the difference between IPSO and PSO appears too minor as shown in Figure 2, but it
has a significant impact to the performance of MPPT in PV systems. The eigen-values
obtained by both optimization algorithms.
Figure 2: Convergence Characteristics of PSO and iteration-PSO based Optimization
2.3 Proposed iterative-PSO based MPPT control algorithm
Basically, PSO algorithms are utilized to solve the optimization problem so that the optimum
result is time invariant. However, in this case, the fitness value (which is the global MPP)
sometimes varies or depends on environmental factors as well as loading states, thus, the
iterative-PSO-based MPPT is utilized in this study and the procedure are as follows;
i. The Iteration-PSO parameters including number of particles (duty cycle) which
cover the search space [dmin, dmax] with equal distance where dmin and dmax are the
minimum and maximum values of the duty cycle of the dc-dc converter
respectively, the weighting factors, c1, c2, and c3 and the maximum number of
iteration are initialized.
ii. Initialize the Iteration-PSO-based MPPT technique is to extract the optimal power
PPV of the photovoltaic system; therefore, the fitness value which is designated as
the generated power is evaluated. The PWM acts according to the particle position
i that denotes the duty cycle state; then the PV voltage VPV and current IPV can be
measured to calculate the fitness value PPV of particle i, which can then be
utilized.
iii. Initialize Pbest and Gbest and obtain the fitness of each particle in the search
space.
iv. Record and update the velocity of each particle according to equation (3).
v. Record and update the position of each particle according to equation. (2).
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
102
vi. End the program if the displacements between gbest and all the pbests become
lower the 1%; and transfer the best particle, doptimum to the dc-dc converter
otherwise repeat steps iii to v.
Figure 3 shows the flow diagram of the proposed iteration-PSO based MPPT algorithm. The
steps followed for the iteration-PSO algorithm is mostly similar to that of the original PSO;
the slight difference comes from updating the new velocity for ascertaining the new position.
Two convergence criteria are employed in this study. The proposed IPSO-based MPPT
method will terminate and yield the gbest solution if the maximum number of iterations is
attained or if all the particles’ velocities become smaller than a certain threshold. Basically,
PSO algorithms are utilized to solve the optimization difficulty so that the optimum result is
time invariant. However, in this case, the fitness value (which is the global MPP) sometimes
varies or depends on environmental factors as well as loading states. To search for the new
global MPP again in these cases, the particles must be reinitialized.
Iterative-PSO Initialization, no. of
particles np, duty cycle di, velocity
of particle, itermax, i=1;t=1
Iterative-PSO Initialization, no. of
particles np, duty cycle di, velocity
of particle, itermax, i=1;t=1
i > itermaxi > itermax
Update particles’ velocity and
position using Eq. (7), (8).
Update particles’ velocity and
position using Eq. (7), (8).
Pgbest =PiPgbest =Pi
i=i+1i=i+1
i=1, t=t+1i=1, t=t+1
Is particle positions
differ by <1%
Is particle positions
differ by <1%
Output di of the gbestOutput di of the gbest
Measure VPV(i) and IPV(i)Measure VPV(i) and IPV(i)
Send the duty cycle to
converter according to
the position of particle
Send the duty cycle to
converter according to
the position of particle
Calculate the power PPV(i)=VPV(i) x IPV(i)Calculate the power PPV(i)=VPV(i) x IPV(i)
Pbest,i=PiPbest,i=Pi
Is Ppbest,i>PgbestIs Ppbest,i>Pgbest
Is Pi>PbestIs Pi>Pbest
Shading pattern
changed?
Shading pattern
changed?
Yes
Yes
No
No
No
No
Yes
No
Yes
Yes
StartStart
Initiate Iterative-PSO
Figure 3: Flowchart of the proposed iteration-PSO-Based MPPT algorithm.
Considering the change in irradiance and shading pattern to be detected here, the following
constraint is utilized. In the proposed technique, the particles will be reinitialized whenever
the following condition is satisfied as in Equation (8):
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
103
( ) (8)
where Ppv,new is the new PV power, Ppv,old is the PV power at the global MPP of the last
operating point and ( ) is the normalized power tolerance. Its value is set to 10% or
selected as 0.1. Thus, if the normalized power mismatch is larger than 0.1, the samples will
be dispersed on the PV curve; otherwise they remain on the MPP. Figure 4 depicts the
comprehensive flowchart of the proposed system.
G=1W/m2
IPV
VPV
Pattern 1 Pattern 2 Pattern 3
IPV IPV
VPV VPV
G=1 W/m2
G=1 W/m2 G=1 W/m2
G=1 W/m2
G=1 W/m2
G=0.3 W/m2
G=0.3 W/m2
G=0.7 W/m2
G=0.7 W/m2
G=0.6 W/m2
G=0.6 W/m2
G=0.1 W/m2
G=0.1 W/m2
G=0.3 W/m2
G=0.3 W/m2
G=0.4 W/m2
-
- -
G=0.4 W/m2
+
+ +
Figure 4: Layout of PV configurations under study with PSC
2.4 Phenomenon of Irregular Shadow Conditions
A PV module comprises many PV cells either connected in series to produce a higher voltage
or connected in parallel to increase current. Many PV cells are therefore connected either in
series or in parallel to form a PV system. The PV curve of the PV cell would exhibit multiple
MPPs under partial-shading conditions because of the bypass diodes as reported in (Ishaque
et al., 2011; Bastidas-Rodriguez et al, 2014, and Abdulkadir et al., 2012). The PV module
characteristics under irregular-shadow conditions are connected at the module terminal with
bypass diodes were described in Ishaque et al. (2011). In the irregular-shadow pattern, the
shaded portion of the cells acts as a load rather than as a generator and creates the hot shot;
hence, the bypass diodes of these shadowed cells will conduct in order to avert this
undesirable situation (Ganjefar et al., 2014, Eltawil and Zhao 2013). Multiple peaks in the PV
curve would be obtained since the shadowed modules are bypassed. The PV curves that result
when this system is under different shadow conditions are shown in Figure 5.
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
104
Figure 5: P-V characteristic curves of PV system under different shading conditions
Generally speaking, the column of cell that is shelter from the same shadow is classified as a
pattern, as shown in pattern1, pattern2 and pattern3 of Figure 5. As can be seen in the figure,
the global MPP could occur either below or above the voltage range (i.e. either on the left or
right of the PV curve) depending on the type of shadow pattern. For this reason, the
conventional MPPT algorithms will be very difficult to apply directly.
3. Simulation of Results and Discussion
The selection of proper values for algorithm control parameters plays a significant role in
solution’s quality. In order to obtain the best performance, fitness of the objective was
implemented to evaluate the convergence speed of the algorithm in finding the best solution.
It should be noted that the convergence test is performed using the size of population. It is
evidently observed from Figure 2 that the maximum number of iterations needed for IPSO
and conventional PSO are 3 and 10 respectively. The effect of the initial and final values of
cognitive and social components acceleration factors on solution performance are studied by
varying their values. Figure 6 show the MPP searching mechanism by iteration-PSO method
under partial shading.
0 2 4 6 8 10 12 14 16 18 20 22
0
10
20
30
40
50
60
70
80
90
100
110
Voltage (V)
Power(W)
GMPPGMPP
BB
AA
CC
AA
CC
BB
Power(w)Power(w)
Voltage (V)Voltage (V)
Particle is currently tryingParticle is currently trying
Particle tried so farParticle tried so far
Future particleFuture particle
Particle with the best
result so far
Particle with the best
result so far
ConvergingConverging
Inertia
Influence
Inertia
Influence
Pbest
Influence
Pbest
Influence
gbest
Influence
gbest
Influence
PbestPbest
GPGP
Figure 6 The MPP searching mechanism by iteration-PSO method under partial shading.
0 2 4 6 8 10 12 14 16 18 20 22
0
10
20
30
40
50
60
70
80
90
100
110
Voltage (V)
Power(W)
Pattern 3
Pattern 1
Pattern 2
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
105
To demonstrate the effectiveness of the proposed IPSO-based MPPT technique, simulations
is performed appropriately. The simulation model parameters of the PV module are shown in
Table 1.
TABLE 1: Simulation Parameters of ICO-SPC 100 w Photovoltaic
Parameter Value
Maximum Power (Pmax) 100 W
Voltage at Pmax (Vmax) 17.3
Current at Pmax (Imax) 5.79
Open Circuit Voltage (Voc) 20.76
Short Circuit Current (Isc) 6.87
In this paper, the simulations are implemented using the MATLAB Simulink model.
According to the design principle, the specification parameters of the complete IPSO-based
MPPT algorithm are shown in Table 2.
TABLE 2: Simulation Parameter Setting of the IPSO-Based MPPT
Parameter Value
Number of particles 3
Minimum duty cycle 0.02
Maximum duty cycle 0.98
Sampling time 0.1s
Maximum iteration 20
ωmax 1.0
ωmin 0.1
C1, min 1
C1,max 1.2
C2,min 1
C2,max 1.6
As can be seen from Figure 8, tracking time of conventional PSO algorithm is about 0.8 s,
and there is relatively large fluctuation near MPP.
For the rapidly irregular shadow, Figure 7 and Figure 8 has shown the experimental results
for the tracking power of the proposed technique and the conventional PSO respectively
under rapidly irregular shadow conditions. The experiment was conducted under the same
conditions as described in the simulation. It can be seen that the experimental results match
very closely to the simulations. For each condition, the MPP is attained in relatively short
time and exhibits almost zero oscillation in steady state. Hence the correctness of the
proposed technique is validated.
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
106
3311 22 44 55 66 77 88 99 1010
100100
200200
Time (s)Time (s)
Power(w)Power(w)
IPSOIPSO
Figure 7: Simulated power tracked using iteration-PSO algorithm for variation in irradiation
condition
100100
200200
Power(w)Power(w)
3311 22 44 55 66 77 88 99 1010
Time (s)Time (s)
PSOPSO
Figure 8: Simulated power tracked using conventional PSO algorithm for variation in
irradiation condition
On the contrary, the MPP can be quickly tracked if using Iteration PSO technique, its
tracking time is only 0.35 s, which accelerates by 60% compared to the former. These curves
show that PSO based algorithm is capable of reaching the GMPP with lesser time for
convergence. Further the conventional PSO based algorithm produces oscillations in PV
output power for a longer duration when compared to the iteration PSO algorithm.
Also, to further verify the rationality of the proposed technique, the performance of the
proposed iteration PSO MPPT techniques is tested under dynamic environmental conditions
as in Figure 9, Figure 10 and Figure 11 respectively. This dynamic condition was adopted
using the European Efficiency Test EN 50530, which is a newly standard for evaluating the
dynamic performance of PV system. As can be seen in Figure 11, iteration PSO method
adequately tracks the ideal MPP power for the whole dynamic profile (ramps sequence).
However, a consistent deviation between the dotted line (ideal MPP power) and solid line
(actual PV power) is clearly visible.
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
107
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
Insolations
Time (sec)
untitled/Signal Builder2 : Group 1
10001000
300300
Time (s)Time (s)
Insolation(W/m2
)Insolation(W/m2
)
Dwell timeDwell time
Dwell timeDwell time
RampupRampup
RampdownRampdown
Initial settling
time
Initial settling
time
n Repetitionsn Repetitions
Figure 9: Ramp test sequence (low-medium insolation) for the characterization of the MPPT
efficiency under changing insolation conditions
0 0.05 0.1 0.15 0.2 0.25 0.3
0
0.2
0.4
0.6
0.8
1
Insolations
Time (sec)
IncreMental_Conductance_MPPT_Simulation_Model_test/Signal Builder2 : Group 1
2020
4040
6060
8080
100100
X 105
X 105
Irradiance(W/m2
)Irradiance(W/m2
)
Figure 10: The complete dynamic test profile
Figure 11: Performance of iteration-PSO method under dynamic test conditions
Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110
ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng
108
3.1 Experimental results
Test of the MPPT technique, a DC-DC boost converter, a programmable DC power supply
emulated as solar photovoltaic is used as a result of the experimental constraint of educational
laboratory equipment. Figure 12 show the experimental set-up of the iteration-PSO method.
The characteristics generated by the Matlab simulation model of the PV (ICO-SPC-100
watts) are then used to program the programmable DC power supply via interfacing software,
providing the foundation for the experimental work. The DC power supply is able to emulate
solar arrays with its Application Area Programming (AAP) feature which permits the
loading, editing and storing of hundreds of current and voltage values.
Figure 12: Experimental set-up of iteration-PSO method
The PV system had been tested for rapidly irregular shadow condition. This condition would
change the characteristics of photovoltaic array, thereby altering the global maximum point
(GMP) of P–V curve. The result as shown in Figure 7 is the output power of the PV
emulating system of the proposed techniques. Figure 8 shows the conventional PSO has a
slow tracking response time and larger oscillation in the output power because the
conventional PSO failed to reach MPP faster.
4. Conclusion
In this paper, an iteration-PSO based MPPT method for tracking MPP was presented. The
proposed algorithm was studied, and the advantages of this strategy over conventional PSO-
based method were highlighted. The performance of the proposed system was validated using
MATLAB simulation and an experimentation system comprising a digital signal controller, a
boost converter, and a programmable DC power supply emulated as PV simulator. Fast and
accurate performance under different conditions, including irregular shadow condition, was
proven as the main advantage of the proposed algorithm. The performance of the proposed
iteration PSO MPPT techniques is tested under dynamic environmental conditions using the
European Efficiency Test EN 50530. The simulation and experimental results indicate that
the converter can track the MPP of the PV system. The obtained results also confirmed that
the response time of the proposed method is faster compared to the other methods, and the
structure of the algorithm is simple. From these results, it is concluded that the control
scheme can be utilized for reliable and high quality PV systems.
Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under
Irregular Shadow Conditions.
AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng
109
References
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MPPT-Based Control Algorithm for PV System Using iteration-PSO under Irregular shadow Conditions

  • 1. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 Copyright © Faculty of Engineering, University of Maiduguri, Maiduguri, Nigeria. Print ISSN: 1596-2490, Electronic ISSN: 2545-5818, www.azojete.com.ng 97 MPPT-BASED CONTROL ALGORITHM FOR PV SYSTEM USING ITERATION- PSO UNDER IRREGULAR SHADOW CONDITIONS M. Abdulkadir*, A. L. Bukar and B. Modu (Department of Electrical and Electronics Engineering, Faculty of Engineering, University of Maiduguri, Maiduguri, Nigeria) *Corresponding author’s e-mail address: abdulkadirmusa@unimaid.edu.ng; Tel.: 08083831978 Co-authors e-mail address: abbalawan9@gmail.com, engrbb05@hotmail.com. Abstract The conventional maximum power point tracking (MPPT) techniques can hardly track the global maximum power point (GMPP) because the power-voltage characteristics of photovoltaic (PV) exhibit multiple local peaks in irregular shadow, and therefore easily fall into the local maximum power point. These conditions make it very challenging, and to tackle this deficiency, an efficient Iteration Particle Swarm Optimization (IPSO) has been developed to improve the quality of solution and convergence speed of the traditional PSO, so that it can effectively track the GMPP under irregular shadow conditions. This proposed technique has such advantages as simple structure, fast response and strong robustness, and convenient implementation. It is applied to MPPT control of PV system in irregular shadow to solve the problem of multi-peak optimization in partial shadow. In order to verify the rationality of the proposed algorithm, however, recently the dynamic MPPT performance under varying irradiance conditions has been given utmost attention to the PV society. As the European standard EN 50530 which defines the recommended varying irradiance profiles, was released lately, the corresponding researchers have been required to improve the dynamic MPPT performance. This paper tried to evaluate the dynamic MPPT performance using EN 50530 standard. The simulation results show that iterative-PSO method can fast track the global MPP, increase tracking speed and higher dynamic MPPT efficiency under EN 50530 than the conventional PSO. Keywords: Photovoltaic, iteration-PSO, MPPT, Controller, Irregular shadow, EN 50530 1. Introduction In the past decade, the photovoltaic (PV) system has gained wide popularity as a renewable- energy source due to depletion of conventional energy sources as well as the high cost of conventional energy sources and their negative effects on the environment. An essential feature of all PV systems is the efficacy of its maximum power point tracking (MPPT). This technique has drawn immense attention from photovoltaic researchers and industry experts as the most economical means to enhance the photovoltaic system efficiency. MPPT is primarily an operating point co-coordinating the PV module and the DC-DC converter. However, MPPT is not simple and easy to track because of the non-linear I–V characteristics of the PV curve and the effect of partial shading causing the inconsistent in irradiance and temperature. Therefore, tracking the accurate maximum power point (MPP) has been always an intricate issue. The tracking eventually becomes sophisticated when all the PV modules do not experience constant irradiance. Several MPPT techniques have been proposed (Petreus et al., 2010; Ishaque et al., 2011; and Abdulkadir et al., 2012). These methods differ in their accuracy, speed or complexity. (Hossain et al. 2013; Eltawil et al, 2013; and David et al, 2014) reviewed and discussed various techniques. For the partially-shaded condition where the shaded cell in a PV module causes a decrease in power, the conventional MPPT technique becomes invalid due to the PV characteristics becoming more complicated and also displaying multiple MPP. This effect of partial shading has been analyzed by many researchers (La Manna et al., 2014 and Ishaque et al., 2011). (Zegaoui et al, 2011) proposed a two-stage technique to track the global MPP. In
  • 2. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 98 the first stage, the operating point of the PV system moves from the vicinity of the global MPP by estimating the equivalent load line. Then, in the second stage, the incremental conductance method is employed which converges the MPP. However, this method fails to track the global MPP if the global MPP lies on the left of the load line. In (Miyatake et al., 2011), a global stage was employed to locate the regions of the local MPP, while a perturb- and-observe algorithm was employed at the local stage to find the global MPP. A sequential extremum seeking control (ESC)-based MPPT technique was proposed in (Luo et al., 2009) based on approximate modelling and analysis of the characteristics of PV modules under variable partial-shading conditions. However, this method exhibits steady-state error and is system-dependent. (Zang et al. 2012) proposed a PV system which adapts the parallel configuration at a particular cell level so that an individual cell in the PV module can achieve its MPP under partial-shading conditions. The input voltage of this configuration is very low, which may increase the difficulty of designing an appropriate power converter. Moreover, the proposed configuration is only suitable for low power applications. Particle swarm optimization (PSO) has high potential for MPPT due to its simple structure, easy implementation and fast computation capability. Since PSO is based on search optimization in principle, it should be able to locate the MPP for any type of PV curve regardless of environmental variations. The direct control structure was adopted by some researchers for the PSO algorithm, where the positions of the PSO particles are used as the duty cycles. Excellent dynamic tracking speeds under severe partial-shading conditions were able to be handled using the method. Furthermore, the steady state oscillations were found to be exceptionally low. For instance, to track the global point in a constant bus voltage application, the conventional PSO was utilized in (Venugopalan et al., 2013). An analytical expression of the objective functions based on PV current, irradiance and temperature was formulated as in (Miyatake et al., 2011) and the conventional PSO was then utilized to track the MPP. The current-based PSO method was proposed by (Miyatake et al. 2011), where the series inductor current of the boost converter is used as the reference signal to generate the pulse width modulation signals for the switching converter. A repulsive term in the velocity equation of the PSO was also introduced (Phimmasone et al., 2009). (Miyatake et al. 2011) proposed an adaptive perceptive PSO (APPSO)-based MPPT algorithm. Ishaque et al. presented an improved PSO-based MPPT algorithm for PV systems and discussed the advantages of using PSO in conjunction with the direct duty cycle control in detail. However, no system design guidelines and practical design considerations are provided in these papers. (Miyatake et al. 2011) attempted to approach the global MPP using the PSO algorithm. In these investigations, the authors tried to realize centralized MPPT control of the modular (multi-module) PV system (Coelho et al, 2010). These MPPT algorithms have good performance under various partial-shading conditions; however, these methods are only suitable for systems that consist of multiple converters. Therefore, the conventional maximum power point tracking (MPPT) techniques can hardly track the global maximum power point (GMPP) because the power-voltage characteristics of photovoltaic (PV) exhibit multiple local peaks in irregular shadow, and therefore easily fall into the local maximum power point. These conditions make it very challenging, and to tackle this deficiency, an efficient Iteration Particle Swarm Optimization (IPSO) has been
  • 3. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 99 developed to improve the quality of solution and convergence speed of the traditional PSO (Phimmasone et al., 2009, Liu and Liu, 2011), so that it can effectively track the GMPP under irregular shadow conditions. This proposed technique has such advantages as simple structure, fast response and strong robustness, and convenient implementation. It is applied to MPPT control of PV system in irregular shadow to solve the problem of multi-peak optimization in partial shadow. In order to verity the rationality of the proposed algorithm, however, recently the dynamic MPPT performance under varying irradiance conditions has been given utmost attention to the PV society. As the European standard EN 50530 which defines the recommended varying irradiance profiles, was released lately, the corresponding researchers have been required to improve the dynamic MPPT performance. This paper also tries to evaluate the dynamic MPPT performance using EN 50530 standard. The simulation results show that iterative-PSO method can fast track the global MPP, increase tracking speed and higher dynamic MPPT efficiency under EN 50530 than the conventional PSO. 2. Materials and Methods 2.1 Particle Swam Optimization PSO is a stochastic, population-based evolutionary algorithm search method, modelled after the behavior of bird flocks (Miyatake et al., 2007). The PSO algorithm maintains a swarm of individuals (called particles), where each particle represents a candidate solution. Particles follow a simple behavior: they emulate the success of neighboring particles and their own achieved success. The position of a particle is therefore influenced by the best particle (pbest) in a neighborhood, as well as the best solution found by all the particles in the entire population (gbest). The particle position, xi, is adjusted using: (1) where the velocity component, , represents the step size. The velocity is calculated by: ( ) ( ) (2) where denotes the particle position for i; the velocity of the particle at i is represented by vi; the number of iterations is denoted by t; the inertia weight is represented by ω; and are uniformly distributed random variables within [0, 1]; and the cognitive and social coefficients are denoted by , respectively (Venugopalan et al., 2013, Chen et al, 2010). The best position for the storage of the ith particle that has been found so far is denoted by the variable pbest,i and the best position for the storage of all the particles is represented by gbest. Figure 1 depicts the movement of the particle in the optimization process.
  • 4. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 100 Figure 1: Movement of particles in the optimization process 2.2 Iterative Particle Swarm Optimization A new PSO technique is introduced in this paper to mitigate the effect of oscillations in maximum power point tracking power systems. The standard PSO is modified by adding a new directory called Iterative Best (Ibest) to enhance the computational time and the quality of the solution. Ibest is known to be the best value of the fitness function that will be achieved by any agent (particle) in the iteration. A new PSO strategy time varying acceleration coefficient is also introduced. Equation (7) shows the modified form of (3) and is referred to as the Repetitive Particle Swarm Optimization (RPSO) here. ( ) ( ) ( ) (3) where c3 represents the weight of the stochastic acceleration terms that is pulling each agent towards the iteration best. refers to the best value of the fitness function that has been obtained by any agent in the tth iteration during optimization process. The cognitive and social learning factors c1 and c2 in the classical PSO algorithm are usually pre-specified to fixed values of 2.0 basically (Chatteijee et al, 2013, Fu and Tong 2010). This may lead to premature convergence and may allow the particles to wander around the search space due to relatively high values of coefficients. The cognitive and social learning factors c1 and c2 are updated as in equations (4) and (5) Furthermore, the dynamic acceleration constant parameter c3 is introduced and presented in equation (6). ( ) (4) ( ) (5) ( ) ( ( ) ) (6) where t is number of iterations. Therefore, the new velocity update of the proposed algorithm can be updated as follows: ( t t cc if i    11 ,1c ) ( ) ( t t cc if i    22 ,2c ) ( ( )1()(c )( 13 2  tcct   ) ( )) (7)
  • 5. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 101 Figure 2 depicts the convergence behaviors for the IPSO algorithm fitness over the original PSO, it can be seen that the fitness value of IPSO offers better result as compared to the original PSO. Not only that, IPSO also convergence faster with attractive result (3rd iteration) compared to the PSO algorithm that required nearly 10th iteration before it converged. Even though the difference between IPSO and PSO appears too minor as shown in Figure 2, but it has a significant impact to the performance of MPPT in PV systems. The eigen-values obtained by both optimization algorithms. Figure 2: Convergence Characteristics of PSO and iteration-PSO based Optimization 2.3 Proposed iterative-PSO based MPPT control algorithm Basically, PSO algorithms are utilized to solve the optimization problem so that the optimum result is time invariant. However, in this case, the fitness value (which is the global MPP) sometimes varies or depends on environmental factors as well as loading states, thus, the iterative-PSO-based MPPT is utilized in this study and the procedure are as follows; i. The Iteration-PSO parameters including number of particles (duty cycle) which cover the search space [dmin, dmax] with equal distance where dmin and dmax are the minimum and maximum values of the duty cycle of the dc-dc converter respectively, the weighting factors, c1, c2, and c3 and the maximum number of iteration are initialized. ii. Initialize the Iteration-PSO-based MPPT technique is to extract the optimal power PPV of the photovoltaic system; therefore, the fitness value which is designated as the generated power is evaluated. The PWM acts according to the particle position i that denotes the duty cycle state; then the PV voltage VPV and current IPV can be measured to calculate the fitness value PPV of particle i, which can then be utilized. iii. Initialize Pbest and Gbest and obtain the fitness of each particle in the search space. iv. Record and update the velocity of each particle according to equation (3). v. Record and update the position of each particle according to equation. (2).
  • 6. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 102 vi. End the program if the displacements between gbest and all the pbests become lower the 1%; and transfer the best particle, doptimum to the dc-dc converter otherwise repeat steps iii to v. Figure 3 shows the flow diagram of the proposed iteration-PSO based MPPT algorithm. The steps followed for the iteration-PSO algorithm is mostly similar to that of the original PSO; the slight difference comes from updating the new velocity for ascertaining the new position. Two convergence criteria are employed in this study. The proposed IPSO-based MPPT method will terminate and yield the gbest solution if the maximum number of iterations is attained or if all the particles’ velocities become smaller than a certain threshold. Basically, PSO algorithms are utilized to solve the optimization difficulty so that the optimum result is time invariant. However, in this case, the fitness value (which is the global MPP) sometimes varies or depends on environmental factors as well as loading states. To search for the new global MPP again in these cases, the particles must be reinitialized. Iterative-PSO Initialization, no. of particles np, duty cycle di, velocity of particle, itermax, i=1;t=1 Iterative-PSO Initialization, no. of particles np, duty cycle di, velocity of particle, itermax, i=1;t=1 i > itermaxi > itermax Update particles’ velocity and position using Eq. (7), (8). Update particles’ velocity and position using Eq. (7), (8). Pgbest =PiPgbest =Pi i=i+1i=i+1 i=1, t=t+1i=1, t=t+1 Is particle positions differ by <1% Is particle positions differ by <1% Output di of the gbestOutput di of the gbest Measure VPV(i) and IPV(i)Measure VPV(i) and IPV(i) Send the duty cycle to converter according to the position of particle Send the duty cycle to converter according to the position of particle Calculate the power PPV(i)=VPV(i) x IPV(i)Calculate the power PPV(i)=VPV(i) x IPV(i) Pbest,i=PiPbest,i=Pi Is Ppbest,i>PgbestIs Ppbest,i>Pgbest Is Pi>PbestIs Pi>Pbest Shading pattern changed? Shading pattern changed? Yes Yes No No No No Yes No Yes Yes StartStart Initiate Iterative-PSO Figure 3: Flowchart of the proposed iteration-PSO-Based MPPT algorithm. Considering the change in irradiance and shading pattern to be detected here, the following constraint is utilized. In the proposed technique, the particles will be reinitialized whenever the following condition is satisfied as in Equation (8):
  • 7. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 103 ( ) (8) where Ppv,new is the new PV power, Ppv,old is the PV power at the global MPP of the last operating point and ( ) is the normalized power tolerance. Its value is set to 10% or selected as 0.1. Thus, if the normalized power mismatch is larger than 0.1, the samples will be dispersed on the PV curve; otherwise they remain on the MPP. Figure 4 depicts the comprehensive flowchart of the proposed system. G=1W/m2 IPV VPV Pattern 1 Pattern 2 Pattern 3 IPV IPV VPV VPV G=1 W/m2 G=1 W/m2 G=1 W/m2 G=1 W/m2 G=1 W/m2 G=0.3 W/m2 G=0.3 W/m2 G=0.7 W/m2 G=0.7 W/m2 G=0.6 W/m2 G=0.6 W/m2 G=0.1 W/m2 G=0.1 W/m2 G=0.3 W/m2 G=0.3 W/m2 G=0.4 W/m2 - - - G=0.4 W/m2 + + + Figure 4: Layout of PV configurations under study with PSC 2.4 Phenomenon of Irregular Shadow Conditions A PV module comprises many PV cells either connected in series to produce a higher voltage or connected in parallel to increase current. Many PV cells are therefore connected either in series or in parallel to form a PV system. The PV curve of the PV cell would exhibit multiple MPPs under partial-shading conditions because of the bypass diodes as reported in (Ishaque et al., 2011; Bastidas-Rodriguez et al, 2014, and Abdulkadir et al., 2012). The PV module characteristics under irregular-shadow conditions are connected at the module terminal with bypass diodes were described in Ishaque et al. (2011). In the irregular-shadow pattern, the shaded portion of the cells acts as a load rather than as a generator and creates the hot shot; hence, the bypass diodes of these shadowed cells will conduct in order to avert this undesirable situation (Ganjefar et al., 2014, Eltawil and Zhao 2013). Multiple peaks in the PV curve would be obtained since the shadowed modules are bypassed. The PV curves that result when this system is under different shadow conditions are shown in Figure 5.
  • 8. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 104 Figure 5: P-V characteristic curves of PV system under different shading conditions Generally speaking, the column of cell that is shelter from the same shadow is classified as a pattern, as shown in pattern1, pattern2 and pattern3 of Figure 5. As can be seen in the figure, the global MPP could occur either below or above the voltage range (i.e. either on the left or right of the PV curve) depending on the type of shadow pattern. For this reason, the conventional MPPT algorithms will be very difficult to apply directly. 3. Simulation of Results and Discussion The selection of proper values for algorithm control parameters plays a significant role in solution’s quality. In order to obtain the best performance, fitness of the objective was implemented to evaluate the convergence speed of the algorithm in finding the best solution. It should be noted that the convergence test is performed using the size of population. It is evidently observed from Figure 2 that the maximum number of iterations needed for IPSO and conventional PSO are 3 and 10 respectively. The effect of the initial and final values of cognitive and social components acceleration factors on solution performance are studied by varying their values. Figure 6 show the MPP searching mechanism by iteration-PSO method under partial shading. 0 2 4 6 8 10 12 14 16 18 20 22 0 10 20 30 40 50 60 70 80 90 100 110 Voltage (V) Power(W) GMPPGMPP BB AA CC AA CC BB Power(w)Power(w) Voltage (V)Voltage (V) Particle is currently tryingParticle is currently trying Particle tried so farParticle tried so far Future particleFuture particle Particle with the best result so far Particle with the best result so far ConvergingConverging Inertia Influence Inertia Influence Pbest Influence Pbest Influence gbest Influence gbest Influence PbestPbest GPGP Figure 6 The MPP searching mechanism by iteration-PSO method under partial shading. 0 2 4 6 8 10 12 14 16 18 20 22 0 10 20 30 40 50 60 70 80 90 100 110 Voltage (V) Power(W) Pattern 3 Pattern 1 Pattern 2
  • 9. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 105 To demonstrate the effectiveness of the proposed IPSO-based MPPT technique, simulations is performed appropriately. The simulation model parameters of the PV module are shown in Table 1. TABLE 1: Simulation Parameters of ICO-SPC 100 w Photovoltaic Parameter Value Maximum Power (Pmax) 100 W Voltage at Pmax (Vmax) 17.3 Current at Pmax (Imax) 5.79 Open Circuit Voltage (Voc) 20.76 Short Circuit Current (Isc) 6.87 In this paper, the simulations are implemented using the MATLAB Simulink model. According to the design principle, the specification parameters of the complete IPSO-based MPPT algorithm are shown in Table 2. TABLE 2: Simulation Parameter Setting of the IPSO-Based MPPT Parameter Value Number of particles 3 Minimum duty cycle 0.02 Maximum duty cycle 0.98 Sampling time 0.1s Maximum iteration 20 ωmax 1.0 ωmin 0.1 C1, min 1 C1,max 1.2 C2,min 1 C2,max 1.6 As can be seen from Figure 8, tracking time of conventional PSO algorithm is about 0.8 s, and there is relatively large fluctuation near MPP. For the rapidly irregular shadow, Figure 7 and Figure 8 has shown the experimental results for the tracking power of the proposed technique and the conventional PSO respectively under rapidly irregular shadow conditions. The experiment was conducted under the same conditions as described in the simulation. It can be seen that the experimental results match very closely to the simulations. For each condition, the MPP is attained in relatively short time and exhibits almost zero oscillation in steady state. Hence the correctness of the proposed technique is validated.
  • 10. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 106 3311 22 44 55 66 77 88 99 1010 100100 200200 Time (s)Time (s) Power(w)Power(w) IPSOIPSO Figure 7: Simulated power tracked using iteration-PSO algorithm for variation in irradiation condition 100100 200200 Power(w)Power(w) 3311 22 44 55 66 77 88 99 1010 Time (s)Time (s) PSOPSO Figure 8: Simulated power tracked using conventional PSO algorithm for variation in irradiation condition On the contrary, the MPP can be quickly tracked if using Iteration PSO technique, its tracking time is only 0.35 s, which accelerates by 60% compared to the former. These curves show that PSO based algorithm is capable of reaching the GMPP with lesser time for convergence. Further the conventional PSO based algorithm produces oscillations in PV output power for a longer duration when compared to the iteration PSO algorithm. Also, to further verify the rationality of the proposed technique, the performance of the proposed iteration PSO MPPT techniques is tested under dynamic environmental conditions as in Figure 9, Figure 10 and Figure 11 respectively. This dynamic condition was adopted using the European Efficiency Test EN 50530, which is a newly standard for evaluating the dynamic performance of PV system. As can be seen in Figure 11, iteration PSO method adequately tracks the ideal MPP power for the whole dynamic profile (ramps sequence). However, a consistent deviation between the dotted line (ideal MPP power) and solid line (actual PV power) is clearly visible.
  • 11. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 107 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 Insolations Time (sec) untitled/Signal Builder2 : Group 1 10001000 300300 Time (s)Time (s) Insolation(W/m2 )Insolation(W/m2 ) Dwell timeDwell time Dwell timeDwell time RampupRampup RampdownRampdown Initial settling time Initial settling time n Repetitionsn Repetitions Figure 9: Ramp test sequence (low-medium insolation) for the characterization of the MPPT efficiency under changing insolation conditions 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.2 0.4 0.6 0.8 1 Insolations Time (sec) IncreMental_Conductance_MPPT_Simulation_Model_test/Signal Builder2 : Group 1 2020 4040 6060 8080 100100 X 105 X 105 Irradiance(W/m2 )Irradiance(W/m2 ) Figure 10: The complete dynamic test profile Figure 11: Performance of iteration-PSO method under dynamic test conditions
  • 12. Arid Zone Journal of Engineering, Technology and Environment, February, 2017; Vol 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818; www.azojete.com.ng 108 3.1 Experimental results Test of the MPPT technique, a DC-DC boost converter, a programmable DC power supply emulated as solar photovoltaic is used as a result of the experimental constraint of educational laboratory equipment. Figure 12 show the experimental set-up of the iteration-PSO method. The characteristics generated by the Matlab simulation model of the PV (ICO-SPC-100 watts) are then used to program the programmable DC power supply via interfacing software, providing the foundation for the experimental work. The DC power supply is able to emulate solar arrays with its Application Area Programming (AAP) feature which permits the loading, editing and storing of hundreds of current and voltage values. Figure 12: Experimental set-up of iteration-PSO method The PV system had been tested for rapidly irregular shadow condition. This condition would change the characteristics of photovoltaic array, thereby altering the global maximum point (GMP) of P–V curve. The result as shown in Figure 7 is the output power of the PV emulating system of the proposed techniques. Figure 8 shows the conventional PSO has a slow tracking response time and larger oscillation in the output power because the conventional PSO failed to reach MPP faster. 4. Conclusion In this paper, an iteration-PSO based MPPT method for tracking MPP was presented. The proposed algorithm was studied, and the advantages of this strategy over conventional PSO- based method were highlighted. The performance of the proposed system was validated using MATLAB simulation and an experimentation system comprising a digital signal controller, a boost converter, and a programmable DC power supply emulated as PV simulator. Fast and accurate performance under different conditions, including irregular shadow condition, was proven as the main advantage of the proposed algorithm. The performance of the proposed iteration PSO MPPT techniques is tested under dynamic environmental conditions using the European Efficiency Test EN 50530. The simulation and experimental results indicate that the converter can track the MPP of the PV system. The obtained results also confirmed that the response time of the proposed method is faster compared to the other methods, and the structure of the algorithm is simple. From these results, it is concluded that the control scheme can be utilized for reliable and high quality PV systems.
  • 13. Abdulkadir et al.: MPPT-Based Control Algorithm for Pv System Using Iteration-PSO Under Irregular Shadow Conditions. AZOJETE, 13(1):97-110 ISSN 1596-2490; e-ISSN 2545-5818, www.azojete.com.ng 109 References Abdulkadir, M., Samosir, A.S., and Yatim A.H.M. 2012. Modelling and simulation of maximum power point tracking of photovoltaic system in Simulink model, IEEE International Conference on Power and Energy (PECon), 2-5 December 2012, Kota Kinabalu Sabah, Malaysia 325-330. Abdulkadir, M., Samosir, A.S., and Yatim, A.H.M. 2012. Modeling and simulation based approach of photovoltaic system in simulink model, ARPN Journal of Engineering and Applied Sciences, 7: 616-623. Bastidas-Rodriguez, J.D., Franco, E., Petrone, G., Ramos-Paja, CA. and Spagnuolo, G. 2014. Maximum power point tracking architectures for photovoltaic systems in mismatching conditions: a review, IET Power Electronics, 7: 1396-1413. Chatterjee A., Ghoshal S. P., and Mukherjee V., Chaotic ant swarm optimization for fuzzy- based tuning of power system stabilizer, International Journal of Electrical Power and Energy Systems, 33: 657-672. Chen L. R., Tsai C. H., Lin Y. L., and Lai Y. S., 2010. A biological swarm chasing algorithm for tracking the PV maximum power point, IEEE Transactions on Energy Conversion, 25: 484-493. Coelho R. F., Concer F. M., and Martins D. C., 2010. A MPPT approach based on temperature measurements applied in PV systems, Industry Applications (INDUSCON), 2010 9th IEEE/IAS International Conference on IEEE, 1-6. David La Manna., Vigni V. L., E. Sanseverino R., Di Dio V., and Romano P., 2014. Reconfigurable electrical interconnection strategies for photovoltaic arrays: A review, Renewable & Sustainable Energy Reviews, 33: 412-426. Eltawil M. A. and Zhao Z., 2013. MPPT techniques for photovoltaic applications, Renewable and Sustainable Energy Reviews, 25: 793-813. Fu Q. and Tong N., 2010. A Complex-method-based PSO algorithm for the maximum power point tracking in photovoltaic system, information technology and computer science (ITCS), 2010 second international conference on IEEE, Kiev, 134-137. Ganjefar S., Ghassemi A. A., and Ahmadi M. M., 2014. Improving efficiency of two-type maximum power point tracking methods of tip-speed ratio and optimum torque in wind turbine system using a quantum neural network, Energy, 67: 444-453. Hossain M. K. and Ali M. H., 2013. Overview on maximum power point tracking (MPPT) techniques for photovoltaic power systems, International Review of Electrical Engineering, 8: 1363-1378. Ishaque K., Salam Z., Taheri H., and Shamsudin A., 2011. A critical evaluation of EA computational methods for Photovoltaic cell parameter extraction based on two diode model, Solar Energy, 85: 1768-1779.
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