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IRJET- Investigation of Organic Solar Cell at Different Active Layer Thickness and Suns using GPVDM
1.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1615 Investigation of Organic Solar Cell at different Active Layer Thickness and Suns using GPVDM Kassahun Lewetegn Damena Lecturer at Arba Minch University, Department of Physics, Arba Minch, Ethiopia ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - The organic photovoltaic device has been electrically simulated by GPVDM software model at different active layer width with different value of suns (intensity of light). Organic bulk heterojunction solar cell consists of the mixture of electron donor (P3HT) and electron acceptor (PCBM) materials as active layer, ITO (indium tin oxide) is a transparent electrode, PEDOT: PSS is electron blocking layer and Al is a back electrode. Electrical simulation has been done at different active layer thickness 100,150,200,250 & 300 nm.The simulation for each of the above thickness was repeated for 1suns, 10suns, 20suns, 30suns and 40suns. In this study it has been observed that J-V characteristics are affected by active layer thickness and light intensity (suns). The power conversion efficiency is maximum at active layer thickness of 200nm for the light intensityof1suns, 10suns, 30sunsand a thickness of 100nm for light intensity of 20suns and 40suns. Themaximumshortcircuitcurrentdensityobservedat200nmactive layer thickness for light intensity of 20suns, 30suns and 40suns. Key Words: solar cell, active layer, simulation, suns, power conversion 1. INTRODUCTION In the recent year, the consumption of fossil fuel has been increased due to industrialization, population, and economic development. The over utilization of fossil fuel is lead to the environmental pollution, global warming, resource depletionand energy shortage in the next generation. The world is switch over to utilize the renewable natural resource to produce the power. Renewable energy resources are generating energy from the natural resources such as sunlight, wind hydro, tide, geothermal and biomass. These natural resources are replenished naturally. There are many technologies used to extract the power from these natural resources. Also,manyfactorsareinfluencingtoproducethe powerfromthese natural resourcessuch as atmospheric temperature, pressure, wind speed and climatic condition [1]. Among renewable energy resources, solar energy is the fastest growth in the world in many developed and the developing countries in the last 20 years. There are two types of technology used to convert the solar energy such as solar thermal and solar cell. Solar energy provides the opportunity to generate power without emitting any greenhouse gas. The photovoltaic system technologies have increasing roles in electric power technologies,providingmoresecure power sourcesandpollution- free electric supplies. Photovoltaic power generation system can directly convert solar energy into electrical energy [2]. The research activity and development in photovoltaic field has usuallybeenfocusedonsolarradiationanalysis,efficientoperating strategies, design and sizing of these systems. Cell efficiency can even become a criterion of principal system feasibility. As a basic parameter, cell efficiency serves as an input in calculatingtheoptimal systemconfiguration,e.g.,asa costrelatedtrade-off between the storage unit and its lifetime, photovoltaic size and its efficiency, and finally the demand side [3]. Among the different type of solar cells, organic solar cells based on a bulk heterojunction (BHJ) composites of conjugate polymers P3HT (poly 3-hexylthiophene) and PCBM (phynyl-C70butyricacidmethylester)thatallowthemaximum absorption of light and have been reported among the highest performing material for researchers investigation and studies [4-9] for improving their power conversion efficiencies. In organicsolarcell,bulk heterojunction(BHJ)formedbyaninterpenetrating of a conjugate polymer and electron accepting molecules constitute a very promising route towardscheapandflexiblesolarcells [10-11] as recently exhibited in progress of automated roll-to-roll processing and solar cell stability [12-13]. Therefore, inconsideration the organic solar cell stated and factors affect solar cell efficiency. Thispaper examinesfactorsthat affecting power conversion efficiency of organic solar cells according to scientific literature. These factors are thickness of active layer and light intensity (suns). The investigation was carried on by using GPVDM solar cell simulator. A. Electrical Simulation The electrical simulation has four different layers including the active layer. The layers from top to bottom are ITO/PEDOT:PSS/P3HT:PCBM/Al.This bulk heterojunction solar cell has been done at different active layer thickness for different value of light intensity (suns) by using GPVDM Software. The layers are shown clearly in the figure below.
2.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1616 Figure 1: Electrical simulation window in GPVDM The software was run for the following layer thickness and light intensity (suns) to record the values of power conversion efficiency, fill factor, maximum power, open circuit voltage and short circuit current density. Table 1: Thickness and number of suns of the four layers No. Layer LayerThickness(nm) Number of suns 1 ITO 100 100,150,200,250,300 2 PEDOT:PSS 100 3 P3HT:PCBM (Active layer) 100 150 200 250 300 4 Al 100 Table 2: Parameters set for GPVDM simulation The simulation for different layer thickness and number of suns carried on by setting the following parameters for electrical simulation No Parameters value Units 1 Electron trap density 3.8x1026 m-3eV-1 2 Hole trap density 1.45x1025 m-3eV-1 3 Electron mobility 2.48x10-7 m2V-1s-1 4 Hole mobility 2.48x10-7 m2V-1s-1 5 Trapped electron to free hole 1.32x10-22 m-2 6 Trapped hole to free electron 4.67x10-26 m-2 7 Free electron to trapped electron 2.5x10-20 m-2 8 Free hole to trapped hole 4.86x10-22 m-2 9 Temperature 300 K
3.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1617 10 Shunt Resistance 1.9x105 ohms 11 Series Resistance 19.5 ohms Result and Discussion I. J-V Characteristics at Different light intensity (suns) A. J-V Characteristics curve when the active layer thickness is 100nm Chart- 1: JV curve of organic solar cell for active layer thickness is 100nm The above JV curve was drawn only for 1sun.The different color shows the differentvalueofsuns.Thelightintensity (suns)are 1suns, 10suns, 20suns, 30suns and 40suns.The better performance was observed at 40suns whichindicatedbya yellowcolor. B. J-V Characteristics curve when the active layer thickness is 150nm Chart- 2: JV curve of organic solar cell for active layer thickness is 150nm
4.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1618 C. J-V Characteristics curve when the active layer thickness is 200nm Chart- 3: JV curve of organic solar cell for active layer thickness is 200nm The above graph shows JV curve for the variation of light intensity from 1suns to40suns.Thegoodperformancewasobserved at 40 suns. D. J-V Characteristics curve when the active layer thickness is 250nm Chart- 4: JV curve of organic solar cell for active layer thickness is 250nm
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1619 E. J-V Characteristics curve when the active layer thickness is 300nm Chart- 5: JV curve of organic solar cell for active layer thickness is 300nm II. Power conversion efficiency at different active layer thickness The following table shows the result of fill factor, power conversion efficiency,maximumpower,opencircuitvoltageandshort circuit current density at different light intensity (suns) with the variation of active layer thickness. Table 3: Efficiency affecting factors with different suns Suns Active layer thickness (nm) Fill Factor (au) PCE (%) Max Power (Watt) Voc (V) Jsc (A/m2) 1 100 0.765 3.765 37.646 0.612 80.44 150 0.728 3.769 37.698 0.603 85.86 200 0.681 4.346 43.455 0.602 105.9 250 0.647 4.202 42.026 0.598 108.7 300 0.613 4.101 41.018 0.594 112.6 10 100 0.642 3.517 351.679 0.682 803.8 150 0.573 3.289 328.942 0.673 853.1 200 0.513 3.544 354.393 0.673 1026 250 0.479 3.291 329.104 0.668 1027 300 0.450 3.085 308.511 0.666 1029 20 100 0.532 3.001 600.184 0.703 1605 150 0.472 2.751 550.103 0.693 1681 200 0.414 2.838 567.699 0.695 1974 250 0.389 2.605 521.083 0.689 1938 300 0.373 2.421 484.209 0.687 1892 30 100 0.444 2.535 760.594 0.715 2397 150 0.401 2.313 693.883 0.706 2455 200 0.352 3.337 700.974 0.707 2814 250 0.336 2.143 642.762 0.702 2720 300 0.329 1.987 596.138 0.699 2589
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1620 40 100 0.377 2.161 864.311 0.723 3172 150 0.349 1.972 788.673 0.714 3159 200 0.312 1.969 787.542 0.716 3523 250 0.307 1.813 725.154 0.711 3322 300 0.303 1.686 674.402 0.708 3141 A. Power conversion efficiency for light intensity of 1suns Chart- 6: PCE versus active layer thickness for 1suns The power conversion efficiency as can be seen from the graph increases from 100nm to 200nm and decreases when we go from 200nm to 300nm.This means that the maximum power conversion efficiency observedwhentheactivelayer thicknessis 200nm.
7.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1621 B. Power conversion efficiency for light intensity of 10suns Chart- 7: PCE versus active layer thickness for 10suns Again the maximum power conversion efficiency observed at 200nm of active layer thickness. A fluctuation of PCE observed between 100nm to 200nm but above 200nm the value of PCE shows a sharp decrease. C. Power conversion efficiency for light intensity 20suns Chart- 8: PCE versus active layer thickness for 20suns
8.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1622 The graph generally shows a decrease in the value of PCE for an increase in the active layer thickness, except the variation observed between 150nm and 200nm. D. Power conversion efficiency for light intensity of 30suns Chart- 9: PCE versus active layer thickness for 30suns According to the above graph the maximum power conversion efficiency observed when the active layer thickness is 200nm.Below and above the thickness of 200nm the value of PCE decreases. E. Power conversion efficiency of light intensity 40suns Chart- 10: PCE versus active layer thickness for 40suns
9.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1623 The above graph which is drawn for 40suns indicates that increase of active layer thickness for the light intensity of 40suns brings a decrease in power conversion efficiency. III. Short circuit current density at different active layer thickness A. Short circuit current density for light intensity of 1suns Chart- 11: Current density at different active layer thickness for 1suns The above graph indicates that there is a direct relationship between the active layer thickness and short circuit current density. B. Short circuit current density for light intensity of 10suns Chart- 12: Current density at different active layer thickness for 10suns
10.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1624 The is an increase in the value of short circuit current density from 100nm to 150nm of active layer thickness. This increase is very large from 150nm to 200nm of active layer thickness. Above 200nm there is a very small increase in the value of short circuit current density for a change of layer thickness from 200nm to 300nm. C. Short circuit current density for light intensity of 20suns Chart- 13: Current density at different active layer thickness for 20suns According to the above graph the value of short circuit current increases for an increase of active layerthicknessbutthisvalue that is current density decreases from 200nm to 300nm of active layer thickness. D. Short circuit current density for light intensity of 30suns Chart- 14: Current density at different active layer thickness for 30suns
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1625 Below and above 200nm the value of short circuit current density decreases. This means that the maximum value of curret density observed at 200nm of active layer thickness. E. Short circuit current density for light intensity of 40suns Chart- 15: Current density at different active layer thickness for 40suns The maximum value of short circuit current observed at 200nm for the light intensity of 40suns. Conclusion A change was observed in current density versus voltage graph for the variation of the change in thickness of active layer and light intensity (suns). The maximum result was observed at 40suns for the active layer thickness of 100nm,150nm,200nm,250nm and 300nm.The power conversion efficiency is maximumat activelayerthicknessof 200nmfor the light intensity of 1suns, 10suns,30suns and a thickness of 100nm for light intensity of 20suns and 40suns.The maximum short circuit current density observed at 200nm active layer thickness for light intensity of 20suns,30suns and 40suns.For 1suns and 10suns of light intensity the maximum short current density observedatthe maximumofactivelayerthicknessthat is 300nm. REFERENCES [1] C. Marimuthu, “A Study of Factors Affecting Solar PV Cell through Matlab / Simulink Model This study considers the Grid Interactive Roof Top Solar,” vol. I, no. 1, pp. 21–25, 2017. [2] P. Srivastava, P. Gupta, and A. Singh, “Critical Factors Affecting Efficiency of Maximum Power Point Tracking in Solar Cells,” vol. 7, no. 1, pp. 2010–2015, 2015. [3] D. S. Rajput and K. Sudhakar, “Effect Of Dust On The Performance Of SolarPVPanel,”vol.5,no.2,pp.1083–1086,2013. [4] S.C Jain, M. Willander and V. Kumar, Conducting organic material and devices (Academic, San Diego, (2007). [5] F. Padinger, R. S. Ritterberger, and N. S. Sariciftci, Effects of postproduction treatmentonplasticsolarcells,Adv.Funct. Mater. 13 (2003) 85-88.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1626 [6] Y. Kim, S. Cook, S. M. Tuladhar, S. A. Choulis, J. Nelson, J. R. Durrant, D. D. C. Bradley, M. Giles, I. McCulloch, C. S. Ha, and M. Ree, A strong regioregularity effect in self-organizing conjugated polymer films and high-efficiency polythiophene:fullerene solar cells, Nat. Mater. 5 (2006) 197-203. [7] N. Rastogi , N. Singh , M. Saxena , International Journal of Innovative Research in Science, EngineeringandTechnology Vol. 2, 12, 2013 [8] J. A. Hauch, P. Schilinsky, S. A. Choulis, R. Childers, M. Biele, and C. J. Brabec, Flexible organic P3HT:PCBM bulk- heterojunction modules with more than 1 year outdoor lifetime, Sol. Energy Mater. Sol. Cells 92 (2008) 727-731. [9] C.J. Brabec, N.S. Sariciftci, C. Hummelen, Plastic Solar Cells, Advanced Materials 11 (2001) 15–26. [10] S.H. Park, A. Roy, S. Beaupre´ , S. Cho, N. Coates, J.S. Moon, D. Moses, M. Leclerc, K.Lee,A.J.Heeger,Bulk heterojunction solar cells with internal quantum efficiency approaching 100%, Nature Photonics 3 (2009) 297–302. [11] Mayer, A.C.; Scully, S.R.; Hardin, B.E.; Rowell, M.W.; McGehee, M.D. “Polymer-based solar cells”. Materials today, Vol.10, No.11, Nov. (2007) pp.28-33 [12] F.C. Krebs, et al., A round robin study of flexible large-area roll-to-roll processed polymer solar cell modules, Solar Energy Material and Solar Cells 93 (2009) 1968–1977 [13] N. Rastogi, N. Singh, Electrical simulation of organicsolarcell atdifferentseriesresistancesanddifferenttemperature IOSR-JAP 8 (2016) 54-57.
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