<?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">CS</journal-id><journal-title-group><journal-title>Circuits and Systems</journal-title></journal-title-group><issn pub-type="epub">2153-1285</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cs.2016.711330</article-id><article-id pub-id-type="publisher-id">CS-71075</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Experimental Processus for Acquisition Automatic Features of I-V Properties and Temperature of the Solar Panel by Changing the Operating Point
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Babou</surname><given-names>Dione</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ousmane</surname><given-names>Sow</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>Mamadou</surname><given-names>Wade</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>L.</surname><given-names>Y. Ibrahima</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Senghane</surname><given-names>Mbodji</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gregoire</surname><given-names>Sissoko</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff4"><addr-line>Université Alioune DIOP de Bambey, Bambey, Sénégal</addr-line></aff><aff id="aff2"><addr-line>University Institute of Technology, University of Thiès, Thiès, Sénégal</addr-line></aff><aff id="aff3"><addr-line>Polytechnic School of Thiès, Thiès, Sénégal</addr-line></aff><aff id="aff1"><addr-line>Laboratory of Semiconductors and Solar Energy, Physics Department, Faculty of Science and Technology, University Cheikh Anta Diop, Dakar, Senegal</addr-line></aff><pub-date pub-type="epub"><day>06</day><month>09</month><year>2016</year></pub-date><volume>07</volume><issue>11</issue><fpage>3984</fpage><lpage>4000</lpage><history><date date-type="received"><day>April</day>	<month>17,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>May</month>	<year>15,</year>	</date><date date-type="accepted"><day>September</day>	<month>30,</month>	<year>2016</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>
 
 
  A development of an acquisition of the characteristic of a solar panel by automatic load variation system is put into play and coupled to an instrumentation chain for taking account of temperature. A programmed digital microprocessor control enables this automation. Design and implementation of a device for automation of variations of the resistive load 
  are 
  powered by solar panel. It is provided by a PIC 16F877A running a computer program that we have developed on the basis of an algorithm according to the operation that we have set. By varying automatically the resistive load, we were able to automatically acquire the characteristic I-V and temperature of the solar panel. With automatic combinations 
  of 
  the 10 resistors, we have obtained 1024 measures of the characteristic curve of the solar cell which has a good accuracy. The change in load and temperature measurement allows us to have the characteristic curves parameterized by temperature.
 
</p></abstract><kwd-group><kwd>Microcontroller</kwd><kwd> Solar Panel</kwd><kwd> Temperature</kwd><kwd> I-V</kwd><kwd> PIC 16F877A</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The use of solar panels as an energy producer has revealed a real need to study it in order to optimize and therefore develop the exploitation of this source of clean renouvenable energy [<xref ref-type="bibr" rid="scirp.71075-ref1">1</xref>] . The research has shown that the functioning of the solar panels is strongly dependent on several parameters: some are external i.e. sunshine and temperature and other internal such as the development of device technology [<xref ref-type="bibr" rid="scirp.71075-ref2">2</xref>] .</p><p>Therefore, the experiment should lead to results similar to the theory [<xref ref-type="bibr" rid="scirp.71075-ref3">3</xref>] .</p><p>Thus, to cope the demand and competition from other energy sources, it is necessary to have a good knowledge on the conversion process of sunlight which will allow designing powerful solar cells and low cost [<xref ref-type="bibr" rid="scirp.71075-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.71075-ref5">5</xref>] .</p><p>Our study focuses on the characteristic I-V and the temperature of a solar cell using an experimental device automatic of the resistive load with a microcontroller [<xref ref-type="bibr" rid="scirp.71075-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.71075-ref7">7</xref>] that is running a C language program code [<xref ref-type="bibr" rid="scirp.71075-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.71075-ref9">9</xref>] .</p><p>With the automation of the change in operating point, based on a mathematical control law, we can impose a particular operation for the study of a phenomenon with given parameters.</p><p>Also we can move from static study to dynamic study with the same experimental device. This work helps to characterize the solar cell to optimize its use.</p></sec><sec id="s2"><title>2. Automatic Change of the Resistive Load of a Solar Panel</title><p>The basic circuit for the characterization of the solar generator is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>We designed a device who gets this characterization so the microcontroller will execute two programs: a program for the static mode and one for the dynamic mode.</p><sec id="s2_1"><title>2.1. Automatic Processus of the Variation of a Resistive Load of a Solar Panel</title><p>We have set up a device consisting of a together of resistor in parallel. Electronic Digital will allow us to remotely control the value of an equivalent electrical resistance [<xref ref-type="bibr" rid="scirp.71075-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.71075-ref11">11</xref>] , which is shown in the following <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>The n resistors into play participate of the association the parallel of resistance following the binary state attributed to them.</p><p>T<sub>i</sub> is a binary number that takes two values: logic zero (0) if the corresponding R<sub>i</sub> is not part in the association or logical (1) if the corresponding R is part of the association. So we have an equivalent resistance that is given by:</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic representation for the characterization of the solar panel</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x2.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Schematic representation for a solar panel automatic characterization</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x3.png"/></fig><disp-formula id="scirp.71075-formula1611"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x4.png"  xlink:type="simple"/></disp-formula><p>Notice that this equivalent resistance is a numerical function given in terms of T<sub>i</sub> [<xref ref-type="bibr" rid="scirp.71075-ref12">12</xref>] .</p><p>This digital function has a countable number N of defined values. The following relationship expresses N in terms of n [<xref ref-type="bibr" rid="scirp.71075-ref9">9</xref>] and is given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x5.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.71075-ref13">13</xref>] .</p><p>We chose as switches of the transistors and this <xref ref-type="fig" rid="fig3">Figure 3</xref> is a schematic of principle characterization [<xref ref-type="bibr" rid="scirp.71075-ref14">14</xref>] .</p><p>So with our transistors that operate in switching mode, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x6.png" xlink:type="simple"/></inline-formula> operating points. Corresponding to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x7.png" xlink:type="simple"/></inline-formula> to our example and thus of 1024 current-voltage couples.</p><p>The equivalent resistance is obtained by the binary signals produced by the sequence and that is applied to the transistors.</p></sec><sec id="s2_2"><title>2.2. The Digital Control Resistance Control Law</title><p>The law of digital control operates using binary signals. So for our example</p><disp-formula id="scirp.71075-formula1612"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x8.png"  xlink:type="simple"/></disp-formula><p>The theory of numbering systems allows us to write [<xref ref-type="bibr" rid="scirp.71075-ref15">15</xref>]</p><disp-formula id="scirp.71075-formula1613"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x9.png"  xlink:type="simple"/></disp-formula><p>This will make that D is a whole integer with value 2<sup>n</sup> defined: 0 &#224;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x10.png" xlink:type="simple"/></inline-formula>which will make 1024 value [<xref ref-type="bibr" rid="scirp.71075-ref4">4</xref>] .</p><p>As D is a function of T and R<sub>&#233;q</sub> also, so we can express R<sub>&#233;q</sub> with D.</p><p>This will allow us to write by asking [<xref ref-type="bibr" rid="scirp.71075-ref8">8</xref>] :</p><disp-formula id="scirp.71075-formula1614"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x11.png"  xlink:type="simple"/></disp-formula><p>We are getting</p><disp-formula id="scirp.71075-formula1615"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x12.png"  xlink:type="simple"/></disp-formula><p>The choice of the value of resistance is arbitrary but we have also taken into account</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Schematic of principle for the solar panel automatic characterization</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x13.png"/></fig><p>standardized commercial values of resistors and the recurrence relation will help us to calculate the others remaining resistance [<xref ref-type="bibr" rid="scirp.71075-ref8">8</xref>] . The recurrence relation is given by this formula:</p><disp-formula id="scirp.71075-formula1616"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x14.png"  xlink:type="simple"/></disp-formula><p>where we have</p><disp-formula id="scirp.71075-formula1617"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x15.png"  xlink:type="simple"/></disp-formula><p>With N = 10, we arbitrarily assigned to the lowest resistance of value 10 and from equation 7 we obtain the following <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The rule is as follows:</p><disp-formula id="scirp.71075-formula1618"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x16.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Acquisition of Temperature</title><p>The choice of the temperature sensor is made on a sensor that does not require external calibrations to give an accuracy of &#177;0.5˚C over a temperature ranging between −40˚C and 85˚C. This sensor is characterized by the equation:</p><disp-formula id="scirp.71075-formula1619"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x17.png"  xlink:type="simple"/></disp-formula><p>The sensor is placed directly on the solar panel. Indeed, according to the technical data we consulted, manufacturers offer solar panels operating in a temperature range between −40˚C and 85˚C. So that with a solar panel whose maximum operating temperature T<sub>max</sub> = 85˚C, we will have a voltage.</p><disp-formula id="scirp.71075-formula1620"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x18.png"  xlink:type="simple"/></disp-formula><p>This voltage is low compared to the voltage which the microcontroller used for conversion which is between 0 - 5 V. In addition to this, the temperature is an analog quantity. The goal is to use all the microcontroller conversion range for better accuracy; we will have to use an amplifier. The characteristic amplifier is adapted to solar panels having operating temperatures between −40˚C and 85˚C. We can look <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Values for resistances regularized</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x19.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x20.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x21.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x22.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x23.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x24.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x25.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x26.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x27.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x28.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >10 Ω</td><td align="center" valign="middle" >20 Ω</td><td align="center" valign="middle" >40 Ω</td><td align="center" valign="middle" >80 Ω</td><td align="center" valign="middle" >160 Ω</td><td align="center" valign="middle" >320 Ω</td><td align="center" valign="middle" >640 Ω</td><td align="center" valign="middle" >1280 Ω</td><td align="center" valign="middle" >2560 Ω</td><td align="center" valign="middle" >5120 Ω</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Diagram of the amplifier</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x29.png"/></fig><p>This amplifier will enable us to achieve a tension close to the microcontroller voltage conversion using its characteristic equation:</p><disp-formula id="scirp.71075-formula1621"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x30.png"  xlink:type="simple"/></disp-formula><p>is the gain of an amplifier</p><disp-formula id="scirp.71075-formula1622"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x31.png"  xlink:type="simple"/></disp-formula><p>So with a solar panel with a maximum operating temperature T<sub>max</sub> = 85˚C, we have:</p><disp-formula id="scirp.71075-formula1623"><graphic  xlink:href="http://html.scirp.org/file/39-7601182x32.png"  xlink:type="simple"/></disp-formula><p>This leads with a voltage of 5 V we will gain: 5 V = 0.85 &#180; G where G = 5.88.</p><p>As the temperature an analog quantity and the peak processes digital data it will have to use a digital to analog converter to pass the signal peak.</p><sec id="s3_1"><title>3.1. Analog/Digital Conversion by the PIC 16F877A</title><p>The analog-digital converter has a resolution of 10 bits. It has eight (8) analog inputs on two (2) ports (PORTA and PORTE). The conversion happens in 2 phases:</p><p>The first time the signal to be converted is applied to the input to convert this signal must be present at least during the time T<sub>acq</sub> (acquisition time of about 20 μS to 5 V).</p><p>The converter is shown schematically in <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>-2nd time: the conversion.</p><p>The minimum conversion time is 12 TAD (TAD is the conversion time depending on the internal clock, typically 1.6 μS).</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Wiring of the analog to digital converter.</title></caption><fig id ="fig5_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x33.png"/></fig></fig-group><p>A conversion always begins by making 1 GO/DONE bit of ADCON0 register. When the conversion is complete this bit back to 0.</p><p>So to read the result in the ADRESL and ADRESH records and just wait that bit GO/DONE changes to 0 [<xref ref-type="bibr" rid="scirp.71075-ref10">10</xref>] .</p><p>The resulting value of the N conversion ADRESH: ADRESL is equal to:</p><disp-formula id="scirp.71075-formula1624"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x34.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x35.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x36.png" xlink:type="simple"/></inline-formula> then</p><disp-formula id="scirp.71075-formula1625"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x37.png"  xlink:type="simple"/></disp-formula><p>But before making a conversion must define the configuration of the converter:</p><p>-The number of analog inputs.</p><p>-The number of digital inputs.</p><p>-The reference of voltage type:</p><p>-Internal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x38.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x39.png" xlink:type="simple"/></inline-formula>.</p><p>-External or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/39-7601182x41.png" xlink:type="simple"/></inline-formula></p><p>Knowing the gain G we can express the temperature according to N noting that V<sub>IN</sub> = V<sub>S</sub> of the amplifier. So we have expression15:</p><disp-formula id="scirp.71075-formula1626"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x42.png"  xlink:type="simple"/></disp-formula><p>Which</p><disp-formula id="scirp.71075-formula1627"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x43.png"  xlink:type="simple"/></disp-formula><p>Replacing G by its value we find</p><disp-formula id="scirp.71075-formula1628"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/39-7601182x44.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Programmable Sequencer of the CNC Resistance</title><p>With a fairly complete calculator, its timers, its reversible digital ports, and its digital to analog converters, our choice was focused on the 16F877 Pic.</p><p> Two output ports to each 8-bit of the microprocessor are cabled of the base resistances of the transistors.</p><p> An input PORT to 8-bit.</p><p> An input PORT at 6-bits for the analog conversion.</p><p> A PORT 8-bit output is wired to the decoders for 7 segment display.</p></sec><sec id="s3_3"><title>3.3. Algorithm for Controlling the Microcontroller PIC 16F877A</title><p>This part is developed a basic algorithm for the study is the static regime is transient dynamic conditions. The choice of plan to study is through a manual switch K. The device is switched on by a push button S. The shutdown of the device is via a pushbutton R that is wired to the microprocessor initialization input. Thus, the system shutdown is not supported by the program resulting from the algorithm. The delay time between two consecutive states is via a button V. The base resistance R<sub>B</sub> is used to fix the current for controlling the switching of the transistors. We schematize our control program in <xref ref-type="fig" rid="fig6">Figure 6</xref>.</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Programmable ordering of processus experimental automatic of solar panel</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x45.png"/></fig><p>Our program is shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>.</p></sec></sec><sec id="s4"><title>4. Experimental Realization of Device</title><p>This work was performed in the laboratory of the Semiconductor and Solar Energy (LASES) of the Faculty of Science and Technology in Dakar. Here is our diagram of the automatic experimental processus for the solar panel which is shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Algorithmic representation of ordering of resistance to digital control</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x46.png"/></fig><p>Our PCB (printed circuit board) is shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>.</p></sec><sec id="s5"><title>5. Presenting Results</title><p>The results are obtained with an analog oscilloscope. The microprocessor PIC 16F877A issued for the controlling part of the automatic experimental. Throughout the manipulation, we calibrated our oscilloscope to 1 V/div for voltage and 0.2 V/div for current and used a temperature sensor to measure the ambient temperature. The following are results taken for different values of the ambient temperature. Figures 10-17 represent the characteristic I-V at different temperature:</p><p>The I-V characteristic in the static mode under illumination polychromatic at 35˚C under an ambient temperature of 33.1˚C.</p><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Diagram of the automatic experimental processes for the solar panel.</title></caption><fig id ="fig8_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x47.png"/></fig><fig id ="fig8_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x48.png"/></fig></fig-group><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> PCB (printed circuit board) artwork of the experimental device</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x49.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 35˚C under an ambient temperature of 33.1˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x50.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 36˚C under an ambient temperature of 33.3˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x51.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 37˚C under an ambient temperature of 32.3˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x52.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 38˚C under an ambient temperature of 33.1˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x53.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 39˚C under an ambient temperature of 33.5˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x54.png"/></fig><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 40˚C under an ambient temperature of 33.1˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x55.png"/></fig><fig id="fig16"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>6</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 42˚C under an ambient temperature of 34.8˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x56.png"/></fig><fig id="fig17"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>7</label><caption><title> Curves I-V characteristic in the static mode under illumination polychromatic at 45˚C under an ambient temperature of 33.8˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x57.png"/></fig><p>The I-V characteristic in the static mode under illumination polychromatic at 36˚C under an ambient temperature of 33.3˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 37˚C under an ambient temperature of 32.3˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 38˚C under an ambient temperature of 33.1˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 39˚C under an ambient temperature of 33.5˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 40˚C under an ambient temperature of 33.1˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 42˚C under an ambient temperature of 34.8˚C.</p><p>The I-V characteristic in the static mode under illumination polychromatic at 45˚C under an ambient temperature of 33.8˚C.</p><p>Here is an example below to calculate current and voltage. Throughout our handling we took 1 V/div for voltage and 0.1 V/div for current see following <xref ref-type="fig" rid="fig1">Figure 1</xref>8.</p></sec><sec id="s6"><title>6. Conclusions</title><p>This work was performed in the laboratory of the Semiconductor and Solar Energy (LASES) of the Faculty of Sciences and Techniques of Dakar.</p><p>It allowed us to design and implement an automatic experimental device for the acquisition of the characteristic I-V and temperature for solar panel silicon.</p><p>The concept of resistance equivalent to several cable resistors in parallel to obtain a digitally controlled variable resistor has been highlighted.</p><p>The electronic binary signals have helped us through static switches considered here as transistors, for changing the wiring resistance of the parallel combination.</p><p>For this we used a microcontroller that executed a C language program.</p><p>The results allowed us to conclude that the change in temperature affects the characteristic I-V. The increase in temperature leads to an increase of the current Icc short</p><fig id="fig18"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>8</label><caption><title> Curves I-V of the solar panel for polychromatic illumination</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/39-7601182x58.png"/></fig><p>circuit and a decrease in the open circuit voltage Voc. Thus it means that the temperature rise causes a slight increase in the creation of electron-hole pairs. Finally the work has allowed us to become familiar with some components such as the microprocessor.</p></sec><sec id="s7"><title>7. Annex</title><p>In this section, we present our execution program of our simulation.</p><p>The program:</p><p>void main() {</p><p>unsigned short int T;</p><p>unsignedint N;</p><p>unsignedint Compteur;</p><p>TRISD=0;</p><p>TRISB=0;</p><p>TRISC.RC0=0;</p><p>TRISC.RC1=0;</p><p>TRISC.RC2=1;</p><p>TRISC.RC3=1;</p><p>TRISA=1;</p><p>ADCON1=0;</p><p>ADCON1.F7=1;</p><p>ADCON0.F6=0;</p><p>ADCON0.F7=1;</p><p>ADCON0.F0=1;</p><p>while (1)</p><p>{</p><p>while (PORTC.RC2==0);</p><p>if (PORTC.RC3==0)</p><p>{ PORTD=0; PORTC=0x01;</p><p>Delay(t3);</p><p>PORTC=0x02;</p><p>Delay(t3); }</p><p>else</p><p>{</p><p>ADCON0.F3=0;</p><p>ADCON0.F4=0;</p><p>ADCON0.F5=0;</p><p>Delay_us(20);</p><p>ADCON0.F2=1;</p><p>while (ADCON0.F2==1);</p><p>N=ADRESL+512*ADRESH.B1+256*ADRESH.B0;</p><p>T=0.084268716081*N;</p><p>if (T&lt;10) PORTB=T;</p><p>else if (T&gt;=10&amp;&amp;T&lt;20) {PORTB=T-10; PORTB.RB4=1;}</p><p>else if (T&gt;=20&amp;&amp;T&lt;30) {PORTB=T-20; PORTB.RB5=1;}</p><p>else if (T&gt;=30&amp;&amp;T&lt;40) {PORTB=T-30; PORTB.RB4=1; PORTB.RB5=1;}</p><p>else if (T&gt;=40&amp;&amp;T&lt;50) {PORTB=T-40; PORTB.RB6=1;}</p><p>else if (T&gt;=50&amp;&amp;T&lt;60) {PORTB=T-50; PORTB.RB4=1; PORTB.RB6=1;}</p><p>else if (T&gt;=60&amp;&amp;T&lt;70) {PORTB=T-60; PORTB.RB5=1; PORTB.RB6=1;}</p><p>else if (T&gt;=70&amp;&amp;T&lt;80) {PORTB=T-70; PORTB.RB5=1; PORTB.RB6=1; PORTB.RB4=1;}</p><p>else if (T&gt;=80&amp;&amp;T&lt;90) {PORTB=T-80; PORTB.RB7=1;}</p><p>else {PORTB=T-90; PORTB.RB4=1; PORTB.RB7=1;}</p><p>PORTD=0;</p><p>PORTC=0;</p><p>Compteur=0;</p><p>while (Compteur&lt;1024)</p><p>{</p><p>if (PORTC.RC4==1)</p><p>Delay(t1);</p><p>else Delay(t2);</p><p>PORTD++;</p><p>if (PORTD==0) PORTC++;</p><p>Compteur++;</p><p>} } } }</p></sec><sec id="s8"><title>Acknowledgements</title><p>The authors gratefully acknowledge the managements of laboratory of the Semiconductor and Solar Energy (LASES) of the Faculty of Sciences and Techniques of Dakar, Polytechnic School of Thi&#232;s, S&#233;n&#233;gal Universit&#233; Alioune DIOP de Bambey, S&#233;n&#233;gal and the University Institute of Technology, University of Thi&#232;s, S&#233;n&#233;gal.</p></sec><sec id="s9"><title>Cite this paper</title><p>Dione, B., Sow, O., Wade, M., Ibrahima, L.Y., Mbodji, S. and Sissoko, G. (2016) Experimental Processus for Acquisition Automatic Features of I-V Properties and Temperature of the Solar Panel by Changing the Operating Point. Circuits and Systems, 7, 3984-4000. http://dx.doi.org/10.4236/cs.2016.711330</p></sec></body><back><ref-list><title>References</title><ref id="scirp.71075-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Sdeepika, P. and Gayad Khan, G.Md. (2014) Analysis of Mathematical Model of PV Cell Module in Matlab/Simulink Environment. International Journal of Advanced Research in Electrical, Electronics and Instrumentation Engineering, 3, 7823-7829.</mixed-citation></ref><ref id="scirp.71075-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Hamrouni, N., Jraidi, M. and Chérif, A. (2008) Solar Radiation and Ambient Temperature Effects on the Performances of a PV Pumping System. 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