<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">WJET</journal-id><journal-title-group><journal-title>World Journal of Engineering and Technology</journal-title></journal-title-group><issn pub-type="epub">2331-4222</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/wjet.2020.83038</article-id><article-id pub-id-type="publisher-id">WJET-102580</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Reliability of the MPPT Control on the Energy Parameters of a Photovoltaic Generator
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Batassou</surname><given-names>Guilzia Jeannot</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mandeng</surname><given-names>Jean Jacques</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mane</surname><given-names>Mane Jeannot</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>University Institute of Technology, UIT, University of Douala, Douala, Cameroon</addr-line></aff><aff id="aff1"><addr-line>Laboratory of Computer and Automatic Engineering, UFD of Engineering Sciences, ENSET, University of Douala, Douala, Cameroon</addr-line></aff><pub-date pub-type="epub"><day>09</day><month>07</month><year>2020</year></pub-date><volume>08</volume><issue>03</issue><fpage>537</fpage><lpage>550</lpage><history><date date-type="received"><day>29,</day>	<month>July</month>	<year>2020</year></date><date date-type="rev-recd"><day>28,</day>	<month>August</month>	<year>2020</year>	</date><date date-type="accepted"><day>31,</day>	<month>August</month>	<year>2020</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  This article describes a technique that allows a photovoltaic (PV) production unit to obtain the maximum power at all times. Here, we use the MPPT control via fuzzy logic on a DC/DC boost-type converter. In order to achieve our goals, we first proceeded to model a PV panel. The resulting model offers the possibility to better account for the influence of different physical quantities such as temperature, irradiation, series resistance, shunt resistance and diode saturation current. Thus, the maximum power to be provided by the PV system is acquired by fuzzification and defuzzification of the input and output variables of the converter. Subsequently, a virtual model of an 800 Watt PV prototype is implemented in the Matlab environment. The simulation results obtained and presented, show the feasibility and efficiency of the proposed technology. Indeed, for a disturbance caused by a variation in brightness, our system guarantees the maximum stable power after 1.4
   
  s. While for a load variation, the maximum power is continuous.
 
</p></abstract><kwd-group><kwd>Low Voltage</kwd><kwd> Photovoltaic System</kwd><kwd> Fuzzy Logic</kwd><kwd> Maximum Power Point</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The incident of 04 November 2006 where Europe was plunged into darkness for an hour, the worst of the general Black-Out, pushed energy suppliers to opt for the integration of decentralized production into low-voltage electricity networks. However, the development of this decentralized production and the liberalization of the electricity market led to many new scientific and technical problems [<xref ref-type="bibr" rid="scirp.102580-ref1">1</xref>]. These problems relate to the geographical structure and management of these modern networks, but they also relate to the optimization of the supply of photovoltaic energy. Several methods have been used to operate the photovoltaic generator (PVG) at its maximum power point (MPP). Among these Maximum Point Power Tracking (MPPT) methods, the P &amp; O Method is essentially a trial and error method [<xref ref-type="bibr" rid="scirp.102580-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.102580-ref3">3</xref>]. This method does not allow the controller to reach its maximum point because of the slowness of the process and the variation in sunlight. On the other hand, the open and short-circuit method [<xref ref-type="bibr" rid="scirp.102580-ref4">4</xref>] has a fast response but cannot always provide the maximum power available due to photovoltaic (PV) characteristics and non-linear atmospheric conditions. Finally, while the Incremental Conductance Algorithm method [<xref ref-type="bibr" rid="scirp.102580-ref5">5</xref>] enables us to find the derivative of the power output of PV, the use of the derived algorithm makes this method unstable. However, Fuzzy Logic Control (FLC) which works like a black box model [<xref ref-type="bibr" rid="scirp.102580-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.102580-ref7">7</xref>] has advantages. It works with imprecise inputs and does not require a precise mathematical model. Moreover, it also handles the non-linearity problem [<xref ref-type="bibr" rid="scirp.102580-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.102580-ref9">9</xref>]. In 2016, Chafiaa Serir et al. [<xref ref-type="bibr" rid="scirp.102580-ref10">10</xref>] used fuzzy logic control to monitor and optimize the multi-source pumping system with the storage battery. Their work focused on system stability to protect the battery from overcharging and deep discharge. Several works have been conducted on this method but in 2019 Belgacem Mbarki et al. [<xref ref-type="bibr" rid="scirp.102580-ref11">11</xref>] did a comparative study on Maximum Power Point Tracking algorithms. Their work was more limited to the ranking of methods used for the determination of the maximum operating point. More recently in 2020 AfshabIlyas et al. [<xref ref-type="bibr" rid="scirp.102580-ref12">12</xref>] worked on the Real-time Implementation of an FPGA-based Fuzzy Logic Controller for Monitoring the Maximum Power Point of the Photovoltaic Solar System.</p><p>The aim of this work is to increase the reliability of the MPPT control over the PV parameters. In this paper, the fuzzy logic method will be used to control the inverter in order to always obtain the maximum power. The remaining sections of the article are organized as follows: In section 2, we describe the method and the materials used. Section 3 is devoted to the results, discussions and comments. Then follows the conclusion.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Materials</title><p>The structure of our photovoltaic system controlled by the MPPT controller is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. It is mainly the photovoltaic modules, DC/DC converter, MPPT controller and load.</p><sec id="s2_1_1"><title>2.1.1. Photovoltaic System Modeling</title><p>The photovoltaic module represented by its equivalent electrical diagram given in <xref ref-type="fig" rid="fig2">Figure 2</xref>, consists of a current source modeling the luminous flux, losses modeled by two resistors, the shunt resistance R<sub>sh</sub>, the series resistance R<sub>S</sub>. In the end, appears in this diagram, the diode for the polarization of the cell and the phenomenon of recombination of minority carriers [<xref ref-type="bibr" rid="scirp.102580-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.102580-ref14">14</xref>].</p><p>The mathematical expressions describing the current-voltage characteristics for different environmental conditions: temperature and irradiation are developed as follows [<xref ref-type="bibr" rid="scirp.102580-ref15">15</xref>]:</p><p>I p v + I D + I s h = I p h (1)</p><p>Or V D = R s h I s h ⇒ I s h = V p v + R S I p v R s h with</p><p>V D = V p v + R S I p v (2)</p><p>and</p><p>I D = I 0 ( exp ( q n K T ( V p v + R S I p v ) ) − 1 ) (3)</p><p>I p v = I p h − I 0 ( exp ( q n K T ( V p v + R S I p v ) ) − 1 ) − V p v + R S I p v R s h (4)</p><p>By asking W ( x ) exp ( W ( x ) ) = x [<xref ref-type="bibr" rid="scirp.102580-ref16">16</xref>] we have:</p><p>I p v = I p h + I 0 − V p v R s h 1 + R S R s h − n V T h R S W [ I 0 R S n V T h ( 1 + R S R s h ) exp ( V p v + ( I p h + I 0 ) R S n V T h ( 1 + R S R s h ) ) ] (5)</p><p>with V T h = K T q .</p><p>On the other hand, the expressions for the photon current, the energy supplied by a cell, and the cell resistances as a function of the temperatures and the effective and standard irradiation are developed by the following equations:</p><p>I p h = [ I s c + K i ( T − T 0 ) ] G G 0 (6)</p><p>I 0 = I p h exp ( V o c N − 1 ) = [ I s c + K i ( T − T 0 ) ] G G 0 exp ( q ( V o c + K v ( T − T 0 ) ) a K T N s ) − 1 (7)</p><p>I s = I 0 ( T T 0 ) 3 exp [ q E g n K ( 1 T − 1 T 0 ) ] (8)</p><p>To obtain the maximum power, the current and the voltage should have their maximum values.</p><p>P max , m = V m p I m p (9)</p><p>Using Equation (4) for the maximum value of the current, Equation (9) becomes:</p><p>P max , m = V m p [ I p h − I 0 ( exp ( q n K T ( V m p + R S I m p ) ) − 1 ) − V m p + R S I m p R s h ] (10)</p><p>Or</p><p>I<sub>pv</sub>: Photovoltaic current (A);</p><p>I<sub>sc</sub>: Short-circuit current (A);</p><p>I<sub>ph</sub>: Light generated current (A);</p><p>K<sub>i</sub>: I<sub>sc</sub> coefficient of temperature (A/˚C);</p><p>K<sub>v</sub>: V<sub>oc</sub> coefficient of temperature (V/˚C);</p><p>E<sub>g</sub>: Gap energy (1.2 eV for crystalline silicon);</p><p>G<sub>0</sub>: Standard lighting (1000 W/m<sup>2</sup>);</p><p>I<sub>0</sub>: Saturation current of the diode (A);</p><p>K: Boltzmann constant (1.381 &#215; 10<sup>−23</sup> J/K);</p><p>R<sub>S</sub> : Series resistance (Ω);</p><p>R<sub>sh</sub>: Parallel resistance (Ω);</p><p>T: Effective cell temperature in kelvin (K);</p><p>T<sub>0</sub>: Standard temperature (1000 W/m<sup>2</sup>).</p><p>Consequently, the physical behavior of the photovoltaic module is related to I p h , I 0 , R S and R s h on the one hand, and on the other hand with two other environmental parameters namely temperature and solar irradiation [<xref ref-type="bibr" rid="scirp.102580-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.102580-ref18">18</xref>].</p></sec><sec id="s2_1_2"><title>2.1.2. DC/DC Converter</title><p>The Boost converter is the most suitable for the PV system, because it has a simple structure and a higher voltage gain than other converters for a given duty cycle [<xref ref-type="bibr" rid="scirp.102580-ref19">19</xref>]. For this reason, we are going to use in our system a step-up chopper which allows to operate the PV generator in such a way as to constantly produce the maximum of its power (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>This converter is governed by the following equations:</p><p>v 0 = 1 1 − D v p v (11)</p><p>i p v = 1 1 − D i 0 (12)</p><p>i L = i p v − c 1 d v p v d t (13)</p><p>i 0 = ( 1 − d ) i L − c 2 d v 0 d t (14)</p><p>where v 0 and i 0 represent respectively the duty cycle, the output voltage and the current of the Boost converter.</p><p>In addition, we will optimize the DC/DC converters used as the interface between the PV generator and the load. This converter allows us to extract the maximum power and to operate this generator at its maximum power point using an MPPT (Maxumun Power Point tracking) controller. As it increases power, the power changes as well as the voltage. These variations are translated by the following equations:</p><p>Δ P p v = P p v ( k ) − P p v ( k − 1 ) (15)</p><p>Δ V p v = V p v ( k ) − V p v ( k − 1 ) (16)</p><p>P p v ( k ) and V p v ( k ) are respectively the power and the voltage of the photovoltaic generator at an instant k.</p></sec><sec id="s2_1_3"><title>2.1.3. Maximum Power Point Tracking</title><p>1) Influence of illumination</p><p>Here we evaluate in Matlab Simulink, the influence of sunlight on the PV system. The model equivalent to a diode of the photovoltaic cell shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> allowed us to obtain Equation (6) of the current photo. Based on this equation, the model of <xref ref-type="fig" rid="fig4">Figure 4</xref> is obtained and the simulation results are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref>.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref> show the current-voltage (I-V) and power-voltage (P-V) curves for different illuminances. The simulation results obtained show that the current photo depends on the solar irradiation. However, as the illuminance increases the current increases while the voltage increases slightly and therefore the power increases.</p><p>2) Influence of temperature</p><p>As the temperature varies according to time and period, we set the interval range [0˚C - 100˚C]. The model in <xref ref-type="fig" rid="fig7">Figure 7</xref> is obtained from Equations (7) and (4), and the simulation results are shown in <xref ref-type="fig" rid="fig8">Figure 8</xref> and <xref ref-type="fig" rid="fig9">Figure 9</xref>.</p><p>For standard illuminance (E = 1 kW/m<sup>2</sup>). It can be seen from <xref ref-type="fig" rid="fig8">Figure 8</xref> and <xref ref-type="fig" rid="fig9">Figure 9</xref> that as the temperature rises, the open circuit voltage V<sub>co</sub> decreases while the short-circuit current I<sub>cc</sub> is relatively constant and therefore the power decreases.</p><p>We notice that the no-load voltage of a module decreases with increasing module temperature while the short-circuit current increases slightly. Thus, the increase in temperature has a negative influence on the power as it decreases. At a constant temperature, the value of the short-circuit current is directly proportional to the radiation intensity. In contrast, the open-circuit voltage does not vary in the same proportion, but remains almost identical. This means that the power of the module is practically proportional to the illuminance. Thus, the power points are at approximately the same voltage.</p></sec></sec><sec id="s2_2"><title>2.2. Methods</title>MPPT Control via Fuzzy Logic<p>Fuzzy logic provides a systematic approach to create the automatic control algorithm by exploiting linguistic variables. In contrast to binary logic, fuzzy variables can ensure a value between 0 and 1. This command has the advantage of being a robust and relatively simple to build [<xref ref-type="bibr" rid="scirp.102580-ref20">20</xref>]. The general structure of FLC is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0 and consists of three steps: fuzzification, inference and defuzzification.</p><p>The purpose of fuzzification is to transform input variables that are initially numerical variables into linguistic variables or scrambled (fuzzy) variables. So we have two input variables, namely the error E(k) and the error variation ∆E(k) defined by the following equations [<xref ref-type="bibr" rid="scirp.102580-ref6">6</xref>]:</p><p>E ( k ) = Δ P p v Δ V p v (17)</p><p>Using Equations (15) and (16) we obtain:</p><p>E ( k ) = P p v ( k ) − P p v ( k − 1 ) V p v ( k ) − V p v ( k − 1 ) (18)</p><p>Δ E ( k ) = E ( k ) − E ( k − 1 ) (19)</p><p>Thus its variables will be denoted Negative Big(NB), Negative Small (NS), Null Error (ZE), Positive Small (PS), Positive Big (PB) [<xref ref-type="bibr" rid="scirp.102580-ref21">21</xref>] (<xref ref-type="fig" rid="fig1">Figure 1</xref>1).</p><p>Inference is a step that allows us to define a logical relationship between input E, ∆E and output D. The truth table described in <xref ref-type="table" rid="table1">Table 1</xref> will allow us to define the membership rules.</p><p>Defuzzification: This step consists in carrying out the inverse operation of fuzzification, i.e. obtaining a numerical value understandable by the external environment (output D) from a fuzzy definition.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>Our fuzzy logic control is developed using the fuzzy toolbox from Matlab/Simulink. The inputs of the fuzzy logic controller are E which shows whether the operating point of the load is located to the left or right of the maximum power bridge and ∆E which shows the direction of the operating point. Their equations are given in (18) and (19). The output of the fuzzy controller D represents the change in the duty cycle of the DC-DC converter. The triangular adhesion functions are chosen for simplicity—they show the fuzzy rule basis created in the current work based on intuitive reasoning and experience. The block diagram for the fuzzy logic controller is shown in Figures 12-14.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Interference matrix</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >E/∆E</th><th align="center" valign="middle" >NB</th><th align="center" valign="middle" >NS</th><th align="center" valign="middle" >ZE</th><th align="center" valign="middle" >PS</th><th align="center" valign="middle" >PB</th></tr></thead><tr><td align="center" valign="middle" >NB</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >NB</td><td align="center" valign="middle" >NB</td><td align="center" valign="middle" >NB</td></tr><tr><td align="center" valign="middle" >NS</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >NS</td><td align="center" valign="middle" >NS</td><td align="center" valign="middle" >NS</td></tr><tr><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >NS</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >PS</td></tr><tr><td align="center" valign="middle" >PS</td><td align="center" valign="middle" >PS</td><td align="center" valign="middle" >PS</td><td align="center" valign="middle" >PS</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td></tr><tr><td align="center" valign="middle" >PB</td><td align="center" valign="middle" >PB</td><td align="center" valign="middle" >PB</td><td align="center" valign="middle" >PB</td><td align="center" valign="middle" >ZE</td><td align="center" valign="middle" >ZE</td></tr></tbody></table></table-wrap><p>After the result in <xref ref-type="fig" rid="fig1">Figure 1</xref>5 allows us to obtain a more stable current. This stability of the current at the maximum operating point is observed from 1.2 s onwards, whereas the current starts to be stable from 1 s onwards. While the voltage starts to be stable from 1.2 s to reach full stability at 1.4 s (<xref ref-type="fig" rid="fig1">Figure 1</xref>6). Compared to the P &amp; O method, we notice that the control by fuzzy logic leads to better performances, with the absence of oscillations in the permanent regimes, and a faster response time. The error is almost non-existent.</p><p>After simulating our system with the fuzzy MPPT control, we find that in the case of a disturbance caused by the change in brightness, the system converges to the MPP and remains stable with a minimal ripple rate compared to other types of control. On the other hand, in the case of a disturbance due to the load, the system is insensitive to the disturbance, the power remains stable and does not fluctuate (<xref ref-type="fig" rid="fig1">Figure 1</xref>7).</p></sec><sec id="s4"><title>4. Conclusion</title><p>This paper proposed a solution to maintain the power at the maximum operating point regardless of irradiation weather and temperature conditions this, by the good of the MPPT control by fuzzy logic. The simulation results are satisfactory for the reliability of the MPPT control over the PV parameters. The support of the DC/DC converter played an important role regarding the stability of the energy. Furthermore, in anticipation of the integration of distributed generation from renewable sources into the power grid, the grid operator will have to impose special conditions for their connection to guarantee the stability and quality</p><p>of the grid. Thus, the development of PV in the LV grid may be the most appropriate solution to reduce peak consumption and participate in the grid service. Although these results are interesting, other perspectives can be considered, i.e. the reduction of the harmonic distortion rate by a DCM-controlled boost converter (duty cycle modulation).</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Jeannot, B.G., Jacques, M.J. and Jeannot, M.M. (2020) Reliability of the MPPT Control on the Energy Parameters of a Photovoltaic Generator. World Journal of Engineering and Technology, 8, 537-550. https://doi.org/10.4236/wjet.2020.83038</p></sec></body><back><ref-list><title>References</title><ref id="scirp.102580-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mutoh, N., Ohno, M. and Inoue, T. (2006) A Method for MPPT Control While Searching for Parameters Corresponding to Weather Conditions for PV Generation Systems. IEEE Transactions on Industrial Electronics, 53, 1055-1065. 
https://doi.org/10.1109/TIE.2006.878328</mixed-citation></ref><ref id="scirp.102580-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Chomsuwan, K., Prisuwanna, P. and Monyakul, V. (2002) Photovoltaic Grid-Con- nected Inverter Using Two-Switch Buck-Boost Converter. Conference Record of the 29th IEEE Photovoltaic Specialists Conference, New Orleans, 19-24 May 2002, 1527-1530. https://doi.org/10.1109/PVSC.2002.1190902</mixed-citation></ref><ref id="scirp.102580-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Xiao, W.D. and Dunford, W.G. (2004) A Modified Adaptive Hill Climbing MPPT Method for Photovoltaic Power Systems. 2004 IEEE 35th Annual Power Electronics Specialists Conference (IEEE Cat. No. 04CH37551), 3, 1957-1963.</mixed-citation></ref><ref id="scirp.102580-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Noguchi, T., Togashi, S. and Nakamoto, R. (2002) Short-Current Pulse-Based Maximum-Power-Point Tracking Method for Multiple Photovoltaic-and-Converter Module System. IEEE Transactions on Industrial Electronics, 49, 217-223. 
https://doi.org/10.1109/41.982265</mixed-citation></ref><ref id="scirp.102580-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Hua, C. and Shen, C. (1998) Comparative Study of Peak Power Tracking Techniques for Solar Storage System. APEC’98 13th Annual Applied Power Electronics Conference and Exposition, Anaheim, 15-19 February 1998, 679-685.</mixed-citation></ref><ref id="scirp.102580-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Messai, A., Mellit, A., Guessoum, A. and Kalogirou, S.A. (2011) Maximum Power Point Tracking Using a GA Optimized Fuzzy Logic Controller and Its FPGA Implementation. Solar Energy, 85, 265-277.  
https://doi.org/10.1016/j.solener.2010.12.004</mixed-citation></ref><ref id="scirp.102580-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Patcharaprakiti, N., Premrudeepreechacharn, S. and Sriuthaisiriwong, Y. (2005) Maximum Power Point Tracking Using Adaptive Fuzzy Logic Control for Grid- Connected Photovoltaic System. Renewable Energy, 30, 1771-1788. 
https://doi.org/10.1016/j.renene.2004.11.018</mixed-citation></ref><ref id="scirp.102580-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Rakpenthai, C., Uatrongjit, S., Watson, N.R. and Premrudeepreechacharn, S. (2013) On Harmonic State Estimation of Power System with Uncertain Network Parameters. IEEE Transactions on Power System, 28, 4829-4838. 
https://doi.org/10.1109/TPWRS.2013.2273943</mixed-citation></ref><ref id="scirp.102580-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Venkateswari, R. and Sreejith, S. (2019) Factors Influencing the Efficiency of Photovoltaic System. Renewable and Sustainable Energy Reviews, 101, 376-394. 
https://doi.org/10.1016/j.rser.2018.11.012</mixed-citation></ref><ref id="scirp.102580-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Serir, C., Rekioua, D., Mezzai N. andBacha, S. (2016) Supervisor Control and Optimization of Multi-Sources Pumping System with Battery Storage. International Journal of Hydrogen Energy, 41, 20974-20986.  
https://doi.org/10.1016/j.ijhydene.2016.05.096</mixed-citation></ref><ref id="scirp.102580-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Mbarki, B. Farhani, F. and Zaafouri, A. (2019) Comparative Study of Some Maximum Power Point Tracking Algorithms. 2019 International Conference on Signal, Control and Communication (SCC), Hammamet, 16-18 December 2019, 145-149.  
https://doi.org/10.1109/SCC47175.2019.9116145</mixed-citation></ref><ref id="scirp.102580-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Ilyas, A., Khan, M.R. and Ayyub, M. (2020) FPGA Based Real-Time Implementation of Fuzzy Logic Controller for Maximum Power Point Tracking of Solar Photovoltaic System. Optik, 213, Article ID: 164668.  
https://doi.org/10.1016/j.ijleo.2020.164668</mixed-citation></ref><ref id="scirp.102580-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Lim, L.H.I., Ye, Z., Ye, J., Yang, D.Z. and Du, H. (2015) A Linear Method to Extract Diode Model Parameters of Solar Panels from a Single I-V Curve. Renewable Energy, 76, 135-142. https://doi.org/10.1016/j.renene.2014.11.018</mixed-citation></ref><ref id="scirp.102580-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Motahhir, S., Ghzizal, A.E. and Derouich, A. (2015) Modélisation et commande d’un panneau photovoltaique dans l’environnement PSIM. fès, Morocco.</mixed-citation></ref><ref id="scirp.102580-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Huang, C., Wang, L., Yeung, R.S.-C., Zhang, Z.J., Chung, H.S.-H. and Bensoussan, A. (2018) A Prediction Model-Guided Jaya Algorithm for the PV System Maximum Power Point Tracking. IEEE Transactions on Sustainable Energy, 9, 45-55. 
https://doi.org/10.1109/TSTE.2017.2714705</mixed-citation></ref><ref id="scirp.102580-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Jain, A. and Kapoor, A. (2004) Exact Analytical Solutions of the Parameters of Real Solar Cells Using Lambert W-Function. Solar Energy Materials and Solar Cells, 81, 269-277. https://doi.org/10.1016/j.solmat.2003.11.018</mixed-citation></ref><ref id="scirp.102580-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Shekoofa, O. and Taherbaneh, M. (2007) Modelling of Silicon Solar Panel by MATLAB/Simulink and Evaluating the Importance of Its Parameters in a Space Application. 2007 3rd International Conference on Recent Advances in Space Technologies, Istanbul, 14-16 June 2007, 719-724. 
https://doi.org/10.1109/RAST.2007.4284087</mixed-citation></ref><ref id="scirp.102580-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Villalva, M.G., Gazoli, J.R. and Filho, E.R. (2009) Comprehensive Approach to Modeling and Simulation of Photovoltaic Arrays. IEEE Transactions on Power Electronics, 24, 1198-1208. https://doi.org/10.1109/TPEL.2009.2013862</mixed-citation></ref><ref id="scirp.102580-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Narendra, A., Naik, N.V., Panda, A.K. and Tiwary, N. (2020) A Comprehensive Review of PV Driven Electrical Motors. Solar Energy, 195, 278-303.  
https://doi.org/10.1016/j.solener.2019.09.078</mixed-citation></ref><ref id="scirp.102580-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Verma, P., Garg, R. and Mahajan, P. (2020) Asymmetrical Interval Type-2 Fuzzy Logic Control Based MPPT Tuning for PV System under Partial Shading Condition. ISA Transactions, 100, 251-263. https://doi.org/10.1016/j.isatra.2020.01.009</mixed-citation></ref><ref id="scirp.102580-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Salam, Z., Ahmed, J. and Merugu, B.S. (2013) The Application of Soft Computing Methods for MPPT of PV System: A Technological and Status Review. Applied Energy, 107, 135-148. https://doi.org/10.1016/j.apenergy.2013.02.008</mixed-citation></ref></ref-list></back></article>