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针对目前太阳位置检测系统精度不高的情况,设计了一种基于CMOS图像传感器和ARM11微控制器的高精度太阳位置检测系统。该系统可以实时采集太阳图像、定时保存图像并对保存的图像进行图像处理、计算太阳光斑圆心偏离图像中心的偏差角,计算所得的数据可以显示在系统界面上。将系统所得太阳偏差角传送到太阳能板转台控制器中,转台控制器调整太阳能板位置使太阳能板正对太阳,从而提高太阳能利用率。实验结果表明,该系统测量精度高、误差小。 相似文献
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为了提高太阳能的利用率,设计一种太阳能自动跟踪控制系统,本系统采用双光电传感器精确定位太阳与太阳能利用装置相对位置,通过单片机智能控制,实现太阳能利用装置的全程太阳追踪;并设计合理的机械结构,通过硬件控制系统,来实现高精度的太阳跟踪.同时,在阴晴不定的天气状况下仍可以实现对太阳的跟踪.具有设计简单、抗干扰能力强、系统控制器稳定、数据传输可靠性高等特点. 相似文献
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高精度太阳能跟踪控制器 总被引:1,自引:0,他引:1
针对目前采用的传统太阳能跟踪控制器传感器形式单一、抗干扰性差、跟踪精度不高等问题,设计了一种基于可编程逻辑控制器(Programmable Logic Controller,PLC)的太阳能跟踪控制器系统。该系统将固定轨迹粗略跟踪方式与光电传感器精确跟踪方式有效地结合起来,并重点将光电传感器加以改进,从而有效地提高了太阳能利用率。由伺服电机作为执行机构控制太阳能板对太阳位置的跟踪,可以实现对太阳高度角和方位角的双自由度跟踪,使太阳能跟踪装置始终正对着太阳光线位置。通过对比实验表明,该跟踪控制器可以达到较高的跟踪精度。 相似文献
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大视场、高精度数字式太阳敏感器 总被引:5,自引:0,他引:5
1 引言 太阳具有离地球近、亮度高、发光均匀等特点,把它作为测量目标,测量太阳矢量在敏感器坐标系中的位置,并将测得的该位置信息提供给卫星姿态控制系统,便可以调整卫星的姿态。表1列出了国内外各类卫星姿态控制系统的构成及性能。由此可以看出,几乎所有的卫星上都用到了太阳敏感器,可见其在姿态控制系统中的重要地位。太阳敏感器的主要类别为0-1式太阳敏感器、模拟式太阳敏感器、数字式太阳敏感器。 相似文献
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提出了一种基于双星敏感器的船体姿态测量系统。本系统采用两台大视场高精度CCD星敏感器,一台指向船艉,一台指向左舷,组合定姿达到提高横摇角测量精度的目的。选用TH7888A作为CCD传感器,成像后经实时图像处理器提取星点目标位置、灰度信息传给数据处理计算机,通过星图识别、姿态确定获取地心惯性坐标系下视轴指向,经岁差、章动、极移、船位、蒙气差等修正,获得惯导地平系下姿态矩阵。依据标定的星敏感器与甲板坐标系安装矩阵,解算船体姿态角,将两台星敏感器解算的姿态角进行融合,达到获取三个高精度船体姿态角的目的。实验表明,该系统航向、纵摇及横摇测角精度分别达到8.46″、7.16″及5.11″,测量精度高、自主性强且能不随时间漂移。 相似文献
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根据地球同步气象卫星 (GSMS)星载扫描同步控制器系统的要求和对太阳目标特性的分析 ,研制了一台用于该GSMS的星载高精度太阳敏感器 (HASS)及配套的性能测试装置 .该太阳敏感器的光学头部由两对狭缝组成 ,采用平衡检测方式产生高精度的太阳脉冲 ,为星上扫描同步控制器和卫星地面站云图配准的引导提供基准信号 .其在卫星子午面内的扇形视场为 - 2 9.5°~ 2 9.5° ,当其随星体按 10 0r/min的速率旋转时 ,可实现 0 .4 6 μs(r.m .s)的测量精度 .另外 ,该太阳敏感器还具有高可靠性、实时性和低功耗的特点 相似文献
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为了提高太阳光伏发电系统的转换效率,对太阳进行自动跟踪是很有必要的。设计一种基于AT89C51单片机的太阳自动跟踪系统。采用程序控制,利用光学传感器对太阳能板做自动定位和误差校正,而通过单片机控制步进电机来实现系统。理论分析和设计结果表明,系统实现了对太阳的自动跟踪,能大大提高太阳能的利用率。该系统价格低廉、性能可靠,具有较高的实用价值。 相似文献
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为了研究抛物面碟形聚光器实现太阳能直接抽运光纤激光器,根据空间太阳光谱分布特点,采用数值方法,计算了用该聚光器聚集太阳能量抽运双包层光纤激光器时光纤吸收的太阳能量及其吸收效率。计算结果表明,通过采用内包层数值孔径较大、掺杂适当稀土元素的双包层光纤及减小太阳光传输过程中的损耗等措施提高光纤激光器对太阳能的吸收效率,可以实现太阳能直接抽运光纤激光器。通过光纤集束熔锥侧面耦合器构成多模光纤阵列或者聚光器阵列的结构,可进一步提高太阳能抽运功率。 相似文献
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Model calculations were performed to investigate and quantify the effect of trap location and trap-assisted Auger recombination on silicon solar cell performance. Trap location has a significant influence on the lifetime behavior as a function of doping and injected carrier concentration in silicon. It Is shown in this paper that for a high quality silicon (τ=10 ms at 200 ohm-cm, no intentional doping), high resistivity (⩾200 ohm-cm) is optimum for high efficiency one sun solar cells if the lifetime limiting trap is located near midgap. However, if the trap is shallow (Et-Ev⩽0.2 eV), the optimum resistivity shifts to about 0.2 ohm-cm. For a low quality silicon material or technology (10 μs at 200 ohm-cm, prior to intentional doping) the optimum base resistivity for one sun solar cells is found to be ~0.2 ohm-cm, regardless of the trap location. It is shown that the presence of a shallow trap can significantly degrade the performance of a concentrator cell fabricated on high-resistivity high-lifetime silicon material because of an undesirable injection level dependence in the carrier lifetime. The effect of trap assisted Auger recombination on the cell performance has also been modelled in this paper. It is found that the trap-assisted Auger recombination does not influence the one sun cell performance appreciably, but can degrade the concentrator cell performance if the trap-assisted Auger recombination coefficient value exceeds 2×10-14 cm3/s. Therefore, it is necessary to know the starting lifetime as well as trap location in order to specify base resistivity in order to predict or achieve the best cell performance for a given one sun or concentrator cell design 相似文献
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Avi Braun Baruch Hirsch Alexis Vossier Eugene A. Katz Jeffrey M. Gordon 《Progress in Photovoltaics: Research and Applications》2013,21(2):202-208
We report experimental results for the effect of irradiance (from 12 up to 8600 suns) on the temperature coefficients of the key performance parameters of multijunction concentrator solar cells, with a flash‐like, real‐sun optical system. Particular attention is paid to the time scales and magnitudes of junction heating, hence the degree to which the cell can be deemed isothermal. The implications for corresponding measurements from solar simulators with pulsed artificial light and for the performance evaluation of concentrator photovoltaics are also addressed. Copyright © 2011 John Wiley & Sons, Ltd. 相似文献
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In this paper, design details, theoretical analysis, and outcomes of a preliminary experimental investigation on a concentrator
thermoelectric generator (CTEG) utilizing solar thermal energy are presented. The designed CTEG system consisted of a parabolic
dish collector with an aperture diameter of 1.8 m used to concentrate sunlight onto a copper receiver plate with 260 mm diameter.
Four BiTe-based thermoelectric cells (TEC) installed on the receiver plate were used to convert the concentrated solar thermal
energy directly into electric energy. A microchannel heat sink was used to remove waste heat from the TEC cold side, and a
two-axis tracking system was used to track the sun continuously. Experimental tests were conducted on individual cells and
on the overall CTEG system under different heating rates. Under maximum heat flux, a single TEC generator was able to produce
4.9 W for a temperature difference of 109°C, corresponding to 2.9% electrical efficiency. The overall CTEG system was able
to produce electric power of up to 5.9 W for a 35°C temperature difference with a hot-side temperature of 68°C. The results
of the investigation help to estimate the potential of the CTEG system and show concentrated thermoelectric generation to
be one of the potential options for production of electric power from renewable energy sources. 相似文献
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《Photovoltaics Bulletin》2003,2003(9):10-11
Spectrolab, a subsidiary of The Boeing Company, announced that it has achieved unprecedented conversion efficiency for a terrestrial concentrator solar cell. Using concentrated sunlight, the photovoltaic cells can convert 36.9% of the sun’s energy to electricity. This technology capability could dramatically reduce the cost of generating electricity from solar energy, according to the California-based company. 相似文献
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I. Antn D. Silva G. Sala A.W. Bett G. Siefer I. Luque‐Heredia T. Trebst 《Progress in Photovoltaics: Research and Applications》2007,15(5):431-447
This paper describes the overall design and experimental results obtained with the PV‐FIBRE concentrator system (CPV). This system uses a parabolic dish to collect and concentrate the sunlight which is then further guided by a transparent rod and finally by individual short fibres. Eventually, the individual fibres are connected to single cells which are located indoors. Dual‐junction III‐V‐based solar cells with an efficiency of 30% and operating at 1000× are applied in the PV‐FIBRE system. This new system approach allows a suitable optical and electrical interconnection in order to reduce the losses and the indoor operation of the cell receiver. All elements of the CPV system (collector, tracker, transmission rod, cells, fibre bundles, and cooling circuit) have been manufactured according to main design requirements and have been evaluated separately. Finally, the PV‐FIBRE CPV system has been installed in Madrid and tested under real operation conditions. The system has demonstrated an optical efficiency of 62% is feasible, providing homogeneous illumination to the cells. Therefore, this concept can lead to overall efficiencies exceeding 20% when combined with MJ solar cells. In this paper we report on the main achievements, identified problems as well as lessons learned and future research lines to improve the system performance. Copyright © 2007 John Wiley & Sons, Ltd. 相似文献
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设计了用于太阳能聚集的全内反射(Total-internal-reflection,TIR)聚光器并采取措施进行优化,将多个TIR聚光器进行叠加放置在光波导板组成波导聚光模块。太阳光线经TIR聚光器阵列收集后照射到光波导板上并在其内部传播,由末端的光伏电池吸收。由实验结果可知,在光波导板长度为400 mm增至4 800 mm的过程中,光学效率由88.6%降低为40.2%,而辐照度由212 W/m2增长为980 W/m2。这样根据不同需求选取不同长度的光波导板,并在保证较高的输出功率的前提下大大减少所需使用的光伏电池面积,同时TIR聚光器只需水平放置在光波导板上,避免了透镜阵列与光波导板的严格对准要求,降低了制造与装配成本。 相似文献