See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/337195909 A review and analysis of technologies applied in PV modules Conference Paper · November 2019 DOI: 10.1109/ISGT-LA.2019.8895369 CITATIONS READS 35 10,750 5 authors, including: Daniel Mesquita João Lucas de Souza Silva State University of Campinas (UNICAMP) State University of Campinas (UNICAMP) 7 PUBLICATIONS 50 CITATIONS 67 PUBLICATIONS 324 CITATIONS SEE PROFILE SEE PROFILE Hugo Moreira Michelle Kitayama da Silva State University of Campinas (UNICAMP) Heriot-Watt University 30 PUBLICATIONS 288 CITATIONS 15 PUBLICATIONS 147 CITATIONS SEE PROFILE All content following this page was uploaded by João Lucas de Souza Silva on 02 December 2019. The user has requested enhancement of the downloaded file. SEE PROFILE A review and analysis of technologies applied in PV modules Marcelo G. Villalva, Member, IEEE Daniel de B. Mesquita, João Lucas de S. Silva, Hugo S. Moreira, Michelle Kitayama School of Electrical and Computer Engineering (FEEC) University of Campinas (Unicamp) Campinas, Brazil Emails: [email protected], [email protected], [email protected], [email protected] Abstract—The implementation of photovoltaic (PV) systems as an alternative source of energy emerges in the electric sector. In this scenario, the challenge arises to present increasingly efficient solutions for PV conversion. As part of these solutions, several types of technology related to PV modules gain prominence in the scientific milieu and in the market dominated by monocrystalline and polycrystalline silicon technologies. Examples are half-cell, double glass, bifacial, PERC, HIT, amorphous silicon, CdTe (cadmium telluride) and CIGS (copper indium gallium selenide) that have the potential for innovation, however, they need to be studied and compared. In this instance, the purpose of this paper is to study the different types of technologies applied in PV modules, verifying the potential of PV conversion of each technology. To evaluate the potential of the technologies, the PV*SOL software was used, limiting an area for the installation of PV modules and simulating the different types of technologies in the limited area. The system with HIT modules presented the best relationship between generated energy and area. HIT technology still presents a high-cost market, meanwhile this technology is expected to be cost-effective in the coming years. Index Terms—PV modules, PV technology, silicon crystalline, thin film I. I NTRODUCTION The photovoltaic (PV) effect that allows the direct conversion of solar energy into electric energy [1], was discovered in 1839 by a french physicist named Alexandre-Edmond Becquerel (1820-1891) [2]. However, it was only in the 1950s that the production of PV cells was initiated by Bell laboratories [3]. Since then, several types of research have been performed on studies of PV cells. With the development of PV technology in the market, in 2017 considering the new implementations of power generation, 40% of the capacity was PV power, between fossil, nuclear, wind, hydro, and other renewable, if continued growth can result until 2025 in the production of 10% of world electricity [4]. Therefore, it is important to continue the evolution with regard to PV devices, always seeking to increase efficiency in the energy conversion process. Regarding to PV modules, the market has the challenge of innovating and adapting to improve the efficiency of energy conversion, increase the useful life and reduce costs. These challenges opened space to several technologies of PV mod- School of Electrical and Computer Engineering (FEEC) University of Campinas (Unicamp) Campinas, Brazil Email: [email protected] ules to emerge in the market which is currently dominated by monocrystalline and polycrystalline silicon technologies. Other technologies such as PERC, half-cell, double glass, bifacial, GaAs and HJT, have the potential for innovation, however, they need to be studied and compared. In this instance, the purpose of this paper is to study the different types of technologies applied to PV modules, verifying the potential of PV conversion of each technology. The study described in this paper, presents and describes the operation of the main PV technologies available in the market, and later uses PV*SOL software, limiting an area for the installation of PV modules and simulating the different types of technologies in the limited area. In this way, it is possible to observe the performance per area of each PV technology, contributing scientifically to the information of which PV technology available in the market has the best generation and area ratio. The paper follows with section II on technologies of PV modules explaining each type of technology, then section III with the description of the simulations, section IV with the results of the simulations and section V with the conclusions obtained in the paper. II. T ECHNOLOGIES OF PHOTOVOLTAIC MODULES This section describes briefly the main technologies of photovoltaic modules available commercially. Currently, technologies derived from crystalline silicon such as monocrystalline, multicrystalline, PERC, half-cell, double glass, bifacial, GaAs and HIT modules account for 90 to 95% of the world market for photovoltaic energy. All thin-film technologies such as amorphous silicon, CdS / CdTe and CIS represent the remainder of the worldwide photovoltaic market [5]. This majority in the market of crystalline silicon technologies is due to the increase of energy conversion efficiency, low cost of production and its reliability. A. Crystalline silicon technologies Silicon (Si) is the second most abundant element in the world, behind only the oxygen (O2) [6]. This material is the main element in the manufacturing process of photovoltaic solar cells with crystalline silicon technology. In the following section, a review on the crystalline silicon technologies is performed. 1) Monocrystalline silicon technology: The monocrystalline silicon is the oldest PV technology. Currently, with this technology, it is possible to obtain an efficiency higher than 25% in laboratory conditions. [7] [8], although, for commercial purposes, the value of efficiency drops slightly, achieving values within 15-22% [9]. The efficiency fluctuates according to the manufacturing process. The majority of the monocrystalline silicon cells are fabricated through the Czochralski process, which was created in 1916 by the folish chemist Jan Czochralski [10]. The fabrication process of the cells require a material purity of 99,9999%. As the electricity conduction of pure silicon is low, a small quantity (parts per million of impurity) of other materials such as boron or phosphorus are added to the cell and therefore the electrical characteristics are changed, thus improving the conduction capacity of the material. Depending on the material added to the mix, the silicon become n-type or p-type. After the fusion stage, a crystal seed is placed at the end of a rotary axis and dipped in silicon. The rotary axis begins to rise slowly turning counterclockwise while the crucible remains fixed, forming a cylindrical silicon ingot.In orfer to the silicon ingot to be considered of good quality it is necessary to have a high control of the temperature gradient, rotation and speed of the process. In addition, it is important that the process is carried out in an inert atmosphere, such as argon, and in an inert chamber [11]. Fig. 1 illustrates the Czochralski process. Fig. 1. Schematic diagram of the Czochralski process [12] The cylindrical ingot is cut into circular waffers for the manufacture of the PV cells that will be used in the manufacture of PV modules. However, the need to save space on the PV module requires that the cylindrical waffers have their edges cut off, transforming into square waffers with their bevelled edges. This process improves the utilization of the space, but causes great waste of the cut and unused material. The aspect of a monocrystalline cell is uniform, usually dark blue or black, and may vary on different color depending on the type of anitireflexive treatment that it receives [13]. Fig.2 illustrates a cell and a monocrystalline module. Fig. 2. Monocrystalline silicon cell and photovoltaic module. 2) Polycrystalline technology: Polycrystalline silicon modules are another technologie derivated from crystalline silicon. These modules have their first efficiency records in 1984. At that time, laboratory tests recorded efficiency values below 15% . Although, nowadays, it is possible to reach efficiency of 22,3% in laboratory environment [7] [8] and for largescale production efficiency is in the range of 14 - 20% [9]. Compared with the monocrystalline technology, one can notice lower efficiency levels. Although, the production costs and the silicon residues generated are also reduced. [14]. The low costs in the manufacturing process of the polycrystalline silicon is due to the fabrication method of block smelting. This method does not need the extraction stage for the formation of the ingot. The silicon is melted and poured in a square coated with SiO/SiN graphite crucible. Next the material undergoes a controlled cooling process which produces a solid block of polycrystalline silicon [15]. Then the block is cut into square waffers for the manufacture of the solar cells. The disadvantage of this method is that the higher polycrystalline silicon contact with the crucible allows a greater transfer of impurity from the crucible to the block of polycrystalline silicon. Thus, polycrystalline cells obtain lower efficiency values compared with monocrystalline cells. However, the fact that the waffers have a square shape make it not necessary to cut the edges of the cells because they are already produced in the ideal geometry for the best use of the space in the modules. Therefore, despite the lower efficiency, compared to monocrystalline cells, the lower manufacturing cost, the smaller amount of residues and the better use of the space in the modules make polycrystalline cells attractive. The Fig. 3 illustrates a polycrystalline cell and module. This technology has the characteristic of presenting a heterogeneous aspect, normally they are found in blue color, but its color can differ according to the antireflexive treatment employed [13]. 3) Half-cell technology: Half-cell is a technology used in the manufacture of photovoltaic modules with high expectation of participating in the market. the ninth edition of the International Technology Roadmap for Photovoltaic (ITRPV) predicts that the participation in the market of the half-cells will increase from 5% in 2018 to almost 40% in 2028 [16]. Conventional crystalline silicon modules have 60 and 72 cells. The half-cell modules have 120 and 144 half-cells, which improves the performance and longevity of the module. The Fig. 5. Conventional module and Double glass module structure, respectively [20]. Fig. 3. Polycrystalline silicon cell and module. cell area directly influences the current of the cell. Therefore, when the cell is cut in half, this half cell will be able to generate a current equivalent to half the current value of a complete cell. Due to current reduction the resistive losses become smaller, allowing the two half cells to produce a little more energy than a complete cell [17]. Manufacturers estimate that half-cell modules have an efficiency gain of 3 % [18]. Another characteristic of the half-cells is the smaller probability of cracks caused by mechanical stress due to the smaller area compared to a complete cell. Therefore, the likelihood of hot spots also decreases. By achieving lower power values, the mandatory spacing between the half cells is less than the complete cell spacing, allowing a better utilization of the module area. The half-cell modules typically use serial-parallel-serial (SPS) connections as shown in the Fig.4. This type of connection allows half-cell modules to have a better response to shading, since one half of the module is not affected by the other. In addition, the SPS connection makes it possible to maintain voltage and current levels similar to the conventional modules [19]. EVA encapsulant degradation, delamination, corrosion in the cell grid line and snail tracks [21]. As a result, the module provides greater mechanical strenghth and durability. 5) Bifacial technology: While conventional modules have an opaque backside, then absorving direct and diffuse irradiance only at the front, the bifacial modules are capable of converting irradiance into electrical energy in both front and backside. There are double glass modules that is possible to observe the backside of the cells, however, to be considered a bifacial module, the cells need to have a metal busbars in both front and backside, as can be seen in the Fig. 6. Fig. 6. Cell and bifacil module. The extra is power output obtained from the back of the module allows a gain of 5 to 30% when compared to a conventional equivalent module, depending on how and where the module installed [22]. According to TUVRheinland [23], the expectation of efficiency gain fluctuates depending on the surface on where the modules were installed as shown in the Table I. Fig. 4. Half-cell module and schematic SPS Connection. 4) Double glass technology: The conventional modules are made with a aluminum frame, front glass, encapsulating EVA, photovoltaic cells, EVA encapsulant, backsheet and junction box. The double glass modules are made with glass on the front, EVA encapsulant, photovoltaic cells, EVA encapsulant, glass on the back and junction box as shown in the Fig. 5. The absence of the metal structure makes the modules less vulnerable to the effect of PID (Potential Induced Degradation). In addition, the glass increases the impermeability of the module, therefore decreasing the moisture hazards such as TABLE I I MPACT OF G ROUND R EFLECTANCE Surface Albedo Water Bare Soil Green grassland, gravel Concrete ground / white gravel Dry / dune sand Reflective roof coatings Fresh snow 5-8% 10-20% Expected yield gain 4-6% 6-8% 15-25% 7-9% 25-35% 8-10% 35-45% 10-15% 80-90% 23-25% 80-95% 25-30% 6) PERC (Passivated Emitter Rear Cell) technology: A conventional crystalline silicon cell does not absorb part of the radiation that arrives at the cell’s surface. This occurs due to the fact that the silicon layer does not absorb all the wavelengths. As a result, some wavelengths surpass all the layers of the silicon until they reach the metalized backside, therefore wasting energy. In order to overcome this problem, the PERC cell is coated between the silicon and the aluminium backside through a dialectric layer that prevents the waste of energy by reflecting the irradiance. This process allows the silicon layers to absorb some wavelengths that would otherwise be wasted, as shown in the Fig. 7. (a) (b) Fig. 7. Structure of: (a) a conventional cell; (b) a PERC cell Due to the recovery of most electrons, the modules with PERC cells reach higher values of current and power. Additionally, they perform better on occasions of low irradiance and lower temperature coefficients. According to [16] [4], there are currently PERC cells which efficiency reached values above 22.5% if they are monocrystalline, and 21% if they are polycrystalline. 7) HIT (heterostructure with intrinsic thin layer) technology: HIT cells are hybrid cells which generally combine crystalline silicon with non-crystalline silicon. As can be seen in the Fig.8, the cells are composed of n-type crystalline silicon with deposition of intrinsic amorphous silicon, amorphous silicon of p-type and n-type. Fig. 8. Structure of a HIT cell [24] These cells combine the advantage of crystalline silicon, such as high efficiency and high stability, with the advantages of amorphous silicon, such as low temperature and relatively less expensive manufacturing process [25]. Thus, these cells reach efficiency levels above 23.7% [16]. Therefore, the modules manufactured with HIT cells are capable of delivering greater output power than other technologies. B. Thin film technologies Thin film photovoltaic modules use less material and manufacturing processes compared with the crystalline silicon [26]. As it requires less material, the solar cell produced by this technology is very thin, around 35 to 260nm [27]. The thin layer of photovoltaic material is placed on a substrate, which is usually glass. For this reason, thin film modules are cheaper, but less efficient than crystalline silicon modules. To compensate the lower efficiency, thin film modules perform better under low irradiance conditions, better aesthetic options, flexibility and light weight. Thin film devices are produced in any size and the only restriction is the base area for manufacturing the module. For this reason the distinction between the cell and module does not exist in modules that use thin film technology [13]. The three major thin film photovoltaic technologies in the market are amorphous silicon, CIGS (Copper Indium Gallium and Selenide) and CdTe (Cadmium Telluride). 1) Amorphous silicon technology: The amorphous silicon technology is the oldest technology in the market of thin film. The amorphous silicon cells are used as a reliable source of energy in electronic equipements such as watches, calculators and others. Among the thin films, the amophous silicon is the one that uses the least amount of material and is less toxic to the producer and consumer [28] [29]. Amorphous silicon is a non-crystalline form of silicon in disordered structure and has a light absorption rate 40 times higher compared to monocrystalline silicon [30]. This disordered structure has a high band gap of 1.7 eV [31], allowing a significant fraction of the light to be absorbed. However, small amounts of amorphous silicon and pendant bonds results in short duration of diffusion of minority carriers and abnormal electrical behavior [28]. Among the three main technologies, amorphous silicon achieves the lowest efficiency. The efficiency of these cells reach values of 14% while the modules achieve efficiency values of 9.8% [7]. 2) CdTe (Cadmium Telluride) technology: The CdTe technology is considered one of the most promissing technologies. It has a bandgap of 1.45 eV, absorbing almost all the visible light and exhibits great thermodynamic stability [32] [33]. These characteristics allow it to reach a better performance compared to crystalline silicon technologies under low-light and high-temperature conditions [34] [35]. However, this technology is more harmful to the environment, and the raw material of this technology is not as abundant as silicon. The manufacturing process of CdTe cells is simpler and cheaper than crystalline silicon and other thin film cells. About 40% of the thin film products available commercially are from CdTe [35] [36]. Cells of this technology reach efficiency levels of 22.1% and their modules reach efficiency values of 18.6% [7]. In a commercial scale, the efficiency is usually 2-4% lower [37]. 3) CIGS (Copper Indium Gallium Selenium) technologies: The manufacturing process of the CIGS cells is performed through vacuum, depositing a thin layer of 2-3 m of copper, TABLE II S IMULATION RESULTS OF THE DIFFERENT TECHNOLOGIES OF PHOTOVOLTAIC MODULES Technology Manufacturer Model Quant. Power Un. (Wp) Power total (kWp) Energy (kWh/Ano) Monocrystalline Monocrystalline Polycrystalline Polycrystalline Polycrystalline Polycrystalline Half-Cell Half-Cell Double Glass Double Glass Bifacial Bifacial PERC PERC HIT CdTe a-Si CIGS Canadian Perlight Canadian Jinko JÁ Solar Perlight Canadian JÁ Solar Canadian JÁ Solar Jinko Longi Jinko Canadian Panasonic First Solar NexPower Global Solar CS6U-330M 1500V PLM-330M-72 CS6U-330P 1500V JKM330P-72 JAP72S01-330/SC PLM-330P-72 CS3U-330P 1500V JAP72S03-330/SC CS6X-330P-FG JAP72D00-330/SC Eagle 72 370Wp LR6-72BP 370M Eagle HC60M 320Wp CS3U-360MS 1500V VBHN330SJ47 FS-4115-3 NT-160AG PowerFLEX-1BTM-300 270 270 270 270 270 270 243 243 270 270 243 216 297 243 288 624 336 144 330 330 330 330 330 330 330 330 330 330 370 370 320 360 330 115 160 300 89,1 89,1 89,1 89,1 89,1 89,1 80,19 80,19 89,1 89,1 89,91 79,92 95,04 87,48 95,04 71,76 53,76 43,2 130104,00 127346,00 131017,00 130239,00 129776,00 126492,00 118353,00 117798,00 130784,00 129631,00 132486,00 119571,00 139384,00 128994,00 144741,00 107963,00 77675,00 60494,00 indium, gallium and selenium on a glass or plastic holder along with electrodes on the front and backside. This deposition can be done on rigid substrates or on flexible substrates, allowing new fields of application and lower manufacturing costs. The band gap of this technology is proportional to the gallium content, ranging from 1.04 eV (pure CuInSe2 ) to 1.68 eV (pure CuGaSe2 ). Higher efficiency cells usually have a band gap of approximately 1.1 to 1.24 eV [38]. Among the major thin-film technologies, CIGS shows the highest potential, achieving efficiencies comparable to polycrystalline silicon cells. [39]. CIGS cells have already registered efficiency values of 22.9% and their modules presented efficiency values of 19.2% [7]. III. D ESCRIPTION OF SIMULATIONS AND RESULTS In order to compare the different types of technology, simulations were performed using the software PV*SOL [40]. The purpose of the simulation was to compare the performance of different modules available commercially and mentioned in this article. The simulations were performed considering the climatic data of Belém-PA, Brazil, as a survey performed by the Comerc Solar Index considering strategic factors (solar irradiance, tax value and energy tariff of the location) concluded that it is considered the best city for installation of new photovoltaic systems in Brazil [41]. In Belém-PA, the annual sum of the global irradiation is 1846 kWh/m2 and the annual average of the temperature is 26.9 o C [40]. Initially, a scenario of a building of 20 meters width 30 meters lenght was created. This building served as the basis for the simulation of all the technologies. For the simulations it was considered installations on slab, in which all the systems were directed to the North (0o orientation), with a slope of 10o and without any shading. For the analysis of the results, some factors were considered, such as the total area, generation by area (GA); specific annual yield (Yf), which represents the relation between the energy Module area (m2 ) 1,944 1,940 1,944 1,940 1,942 1,940 1,984 1,982 1,952 1,952 1,962 1,969 1,652 1,984 1,062 0,720 1,540 2,825 Total area (m2 ) 525,00 523,90 525,00 523,90 524,44 523,80 482,11 481,63 527,11 527,11 476,81 425,32 490,55 482,11 305,99 449,28 517,44 406,81 GA (kWh/Area) Yf (kWh/kWp) PR (%) 247,82 243,08 249,57 248,60 247,46 241,49 245,49 244,58 248,12 245,93 277,86 281,13 284,14 267,56 473,02 240,30 150,11 148,70 1460,20 1429,25 1470,45 1461,71 1456,52 1419,66 1475,90 1468,99 1467,83 1454,89 1473,54 1496,13 1466,58 1474,55 1522,95 1504,51 1444,85 1400,32 80,40% 78,70% 80,90% 80,4% 80,1% 78,1% 81,20% 80,80% 80,70% 80,10% 79,60% 80,90% 80,80% 81,10% 83,70% 82,80% 79,50% 77,40% generated and the nominal power of the photovoltaic system; and the performance ratio (PR) [42]. The simulated modules and their results are shown in Table II. It is worth note that, modules of the same technology and power of different manufacturers present different results, this is due to the quality of the material used and the manufacturing process. Another aspect observed is a higher yield of a polycrystalline module compared to a monocrystalline module of the same manufacturer. This occurs due the fabrication process in large scale of these technologies present similar efficiencies and, because polycrystalline technologies have a better use of the module area, in some cases a better yield is achieved. When it comes to half-cell modules manufactured from polycrystalline cells, the yield was higher than full-cell modules. The improvement of the yield occurs due to the reduction of the resistive losses of the internal connections of the modules. The double glass modules with polycrystalline cells presented a performance similar to the conventional polycrystalline modules. However, the double glass modules present better mechanical resistivity; require less area to obtain the same installed power and a better yield than the conventional modules. This improvement in yield may vary according to the albedo level that reaches the backside of the modules. PERC modules can use a wider range in the radiation spectrum, producing more energy than the conventional modules using the same area. However, the HIT modules achieved the highest energy per area, due to the combination of the advantages of crystalline and non-crystalline silicon. Among the thin film technologies, CdTe presented the best results, followed by amorphous silicon and CIGS, respectively. Although CIGS already achieved better laboratory efficiencies, the industrial manufacturing of CdTe is more consolidated than CIGS, which is still considered a new technology. IV. C ONCLUSION The work presented a review on the types of technologies of photovoltaic modules found in the market, later simulations of systems was performed using the several technologies in order to observe their performances. The system with HIT modules presented the highest value of energy generated and the smallest area used. This technology is recent in the market and its cost is high. However, due to its advantages, it is expected that this technology will have its cost lowered and stands out in the market. ACKNOWLEDGMENT This work was supported by the agencies CNPq, CAPES and ANEEL (CPFL-PA3032). R EFERENCES [1] J. L. D. S. Silva, H. S. Moreira, D. D. B. Mesquita, and M. G. Villalva, “Analysis of Power Optimizers in Photovoltaic Power Plant,” pp. 4–5. [2] H. J. Moller, “SEMICONDUCTORS FOR SOLAR APPLICATIONS,” Middle East, vol. 35, pp. 205–418, 1991. [3] L. 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