• Title/Summary/Keyword: Optimum output voltage of Solar cell

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Tracking System for Optimum Solar Power System of Widely Separated Cave (고립원격지 동굴 전원용 태양광발전 광 추적 시스템)

  • Suh, Oh-Ji;Soh, Dea-Wha
    • Journal of the Speleological Society of Korea
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    • no.89
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    • pp.27-33
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    • 2008
  • Solar energy is most green and clean, unlimited and sustainable energy source on the earth. It is almost 97% of imported consumer energy in Korea. Because of resource poor nation, it is necessary to do their best to make alternative energy to allot their deficiency of the matter in hand of energy resources of petroleum. In a point of view of this problems, the natural solar energy should be improved by any methods as much, possible as we need. Photovoltaic generation with solar tracking system for obtaining optimal power is one of most benefit equipment to improve power of solar-cell panel producing clean electric power efficiently. Solar tracker is a device for orienting a solar photovoltaic panel toward the sun perpendicularly to sunlight, especially in widely separated place. For this reason, we are very interested in developing the equipment system of tracker, specially in solar cell applications, obtaining a high degree of accuracy to ensure that the optimal sunlight could be directed precisely against to the powered device. As a result, it was obtained of 12.46 volts at 90$^\circ$toward solar panel and 9.44 volts at 45$^\circ$, furthermore, improved efficiency more than 30% of average output voltage between tracker system (12.41V) and fixed system (8.55V), respectively. It is also very useful for optimum power system of widely separated cave.

Optimal Voltage Arrangement between PV Array and Battery with minimal energy loss (PV시스템의 Matching 손실저감을 위한 태양전지 및 축전지 최적전압 구성법)

  • 유권종;송진수;강기환;노명근;성세진
    • The Transactions of the Korean Institute of Power Electronics
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    • v.2 no.4
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    • pp.11-18
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    • 1997
  • 태양광 발전시스템의 발전출력은 일사량과 온도에 따라서 크게 변동하고, 태양전지 어레이와 병렬로 연결되는 축전지의 전압에 의해 변동한다. 이 대책으로 지금까지 MPPT 제어(최대출력점 제어)를 해왔는데, 이 제어방식은 손실이 크고 비용이 많이 든다. 따라서 본 논문에서는 이러한 PV 시스템 구성요소의 매칭 손실저감을 위하여 PSpice를 이용한 구성요소의 전자 모델링을 행하고, 태양전지 어레이와 축전지 및 인버터 입력전압의 최적 전압구성법에 대한 연구 결과에 대하여 기술하고 있다. 축전지 최적전압은 태양전지 어레이 최적전압의 약 90%정도가 적당하다는 결과를 얻었다.

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A Study on the Design and Control Characteristics for Optimum Operation of the PV System-based ESS (PV System 기반 ESS의 최적운전을 위한 설계 및 제어 특성에 관한 연구)

  • Cha, Insu;Park, Jongbok;Jung, Gyeonghwan
    • Journal of the Korean Solar Energy Society
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    • v.36 no.5
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    • pp.19-30
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    • 2016
  • In this study, realize voltage regulation $220Vac{\pm}10%$ or less, frequency fluctuation $60Hz{\pm}1%$ or less over the independent operation and grid-connected operation technologies for power stabilization relates to the ESS designed and manufactured in conjunction with solar installations and solar to compensate the output reduction due to the polarization of the solar module through the polarization prevention technology for preventing the optical module efficiency is lowered, in conjunction with the BMS inverter efficiency was more than 92%, more than 90% of the charging efficiency to the target. This study was designed in conjunction with the ESS solar power plants, grid-connected operation and independent operation, Peak-Cut, it can stabilize the grid via the Peak-Shifting operation

Simulation on Optimum Doping Levels in Si Solar Cells

  • Choe, Kwang Su
    • Korean Journal of Materials Research
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    • v.30 no.10
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    • pp.509-514
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    • 2020
  • The two key variables of an Si solar cell, i.e., emitter (n-type window layer) and base (p-type substrate) doping levels or concentrations, are studied using Medici, a 2-dimensional semiconductor device simulation tool. The substrate is p-type and 150 ㎛ thick, the pn junction is 2 ㎛ from the front surface, and the cell is lit on the front surface. The doping concentration ranges from 1 × 1010 cm-3 to 1 × 1020 cm-3 for both emitter and base, resulting in a matrix of 11 by 11 or a total of 121 data points. With respect to increasing donor concentration (Nd) in the emitter, the open-circuit voltage (Voc) is little affected throughout, and the short-circuit current (Isc) is affected only at a very high levels of Nd, exceeding 1 × 1019 cm-3, dropping abruptly by about 12%, i.e., from Isc = 6.05 × 10-9 A·㎛-1, at Nd = 1 × 1019 cm-3 to Isc = 5.35 × 10-9 A·㎛-1 at Nd = 1 × 1020 cm-3, likely due to minority-carrier, or hole, recombination at the very high doping level. With respect to increasing acceptor concentration (Na) in the base, Isc is little affected throughout, but Voc increases steadily, i.e, from Voc = 0.29 V at Na = 1 × 1012 cm-3 to 0.69 V at Na = 1 × 1018 cm-3. On average, with an order increase in Na, Voc increases by about 0.07 V, likely due to narrowing of the depletion layer and lowering of the carrier recombination at the pn junction. At the maximum output power (Pmax), a peak value of 3.25 × 10-2 W·cm-2 or 32.5 mW·cm-2 is observed at the doping combination of Nd = 1 × 1019 cm-3, a level at which Si is degenerate (being metal-like), and Na = 1 × 1017 cm-3, and minimum values of near zero are observed at very low levels of Nd ≤ 1 × 1013 cm-3. This wide variation in Pmax, even within a given kind of solar cell, indicates that selecting an optimal combination of donor and acceptor doping concentrations is likely most important in solar cell engineering.