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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >High efficiency Al-N cermet solar coatings with double cermet layer film structures
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High efficiency Al-N cermet solar coatings with double cermet layer film structures

机译:具有双层金属陶瓷薄膜结构的高效Al-N金属陶瓷太阳能涂料

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A physical model of the optical behaviour of aluminium nitride cermet solar coatings has been used to optimize the metal volume fraction and layer thickness of the coatings. A modified photo-thermal conversion efficiency for solar collector tubes is presented and used. The cermet layers are generally deposited by reactive sputtering in a gas mixture of argon and nitrogen. Sputtered aluminium Al~(sp) is used as a metallic component in the cermet and its refractive index, evaluated in this study, is employed. Due to oxygen contamination, aluminium oxynitride (AlON) is used as a ceramic component in the cermet. Bruggeman approximations are used to calculate the dielectric function for composite materials. An initial ten-layer grade film optimized to one nearly identical to a double cermet film structure when maximizing photo-thermal conversion efficiency at 80°C under a concentration of 1. The optimized films, F10Lm (for initial ten-layer graded film) and F3Lm (for three-layer film) have an identical absorptance of 0.957 and an identical hemispherical emittance of 0.048 at 80°C. The optimized film consists of one anti-reflection layer and two cermet layers with metal volume fractions of 0.093 and 0.255, and thickness of 30 nm and 93 nm, respectively, going from the anti-reflection coating to the infrared reflector layer. The solar performance can be further improved using a lower refractive index anti-reflection layer and a lower emittance infrared reflector. For example, using an Al_2O_3 anti-reflection layer, the solar absorptance increases to 0.974, and using a Cu infrared reflector, hemispherical emittance decreases to 0.033 to 80°C. For these different anti-reflection and infrared reflector materials, optimized calculations have also predicted that the double cermet layer film structures have the highest photo-thermal conversion efficiency.
机译:氮化铝金属陶瓷太阳能涂层光学行为的物理模型已用于优化涂层的金属体积分数和层厚度。提出并使用了改进的太阳能集热管的光热转换效率。金属陶瓷层通常通过反应溅射在氩气和氮气的气体混合物中沉积。溅射铝Al〜(sp)用作金属陶瓷中的金属成分,并采用本研究评估的折射率。由于氧污染,氮氧化铝(AlON)被用作金属陶瓷中的陶瓷成分。 Bruggeman逼近用于计算复合材料的介电函数。当在浓度为1的情况下最大程度地提高80°C的光热转换效率时,将初始十层级薄膜优化为几乎与双层金属陶瓷薄膜结构相同的薄膜。优化薄膜F10Lm(用于初始十层级薄膜)和F3Lm(用于三层膜)在80°C下具有相同的吸收率0.957和相同的半球形发射率0.048。优化的薄膜由一层抗反射层和两层金属陶瓷层组成,金属层的体积分数分别为0.093和0.255,厚度分别为30 nm和93 nm,从抗反射涂层到红外反射层。使用较低折射率的抗反射层和较低发射率的红外反射器可以进一步改善太阳能性能。例如,使用Al_2O_3抗反射层,日吸收率增加到0.974,并且使用Cu红外反射器,半球形发射率减少到0.033至80℃。对于这些不同的抗反射和红外反射器材料,优化计算还预测了双层金属陶瓷层膜结构具有最高的光热转换效率。

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