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首页> 外文期刊>Heat Transfer Research >EMISSIVITY MODEL OF ALUMINUM 6063 WITH AN OXIDE FILM AT A WAVELENGTH OF 1.5 mu m IN THE TEMPERATURE RANGE 800-910 K
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EMISSIVITY MODEL OF ALUMINUM 6063 WITH AN OXIDE FILM AT A WAVELENGTH OF 1.5 mu m IN THE TEMPERATURE RANGE 800-910 K

机译:铝6063的发射率模型,氧化膜在温度范围内为1.5μm的波长为1.5μmk

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This paper models the variation of emissivity with temperature or/and surface oxidation. The emissivity measurements were done at a wavelength of 1.5 mu m over the temperature range from 800 to 910 K. The sample was heated to a certain temperature in air and kept at that temperature for approximately 6 h during the experiment. The radiation was received by an InGaAs detector. The surface temperature of samples was measured by two thermocouples, which were symmetrically welded on the surface of the samples. The average of their readings was regarded as the true temperature. Eleven models were used to investigate the variation of emissivity with growth of an oxide layer on the sample surface at a certain temperature. The effect of the number of parameters used in the models on the fitting quality was evaluated. The fitting quality of the emissivity models with the same number of parameters was compared. The variation of emissivity with temperature was studied at a certain thickness of the oxide film. Three approximate models were used to explore the variation in emissivity with temperature and thickness of the oxide layer, with two of them being found to accurately reproduce the emissivity. The strong oscillations of emissivity were observed during the initial heating period, which were affirmed to arise from the interference effect between the two radiations stemming from the oxide film and coming from the substrate.
机译:本文模拟了温度或/和表面氧化的发射率的变化。在800至910K的温度范围内以1.5μm的波长为1.5μm的发射率测量。将样品加热到空气中的一定温度并在实验期间保持该温度约6小时。辐射由InGaAs检测器接收。通过两个热电偶测量样品的表面温度,其对称地焊接在样品的表面上。他们的读数的平均值被视为真正的温度。使用11个模型来研究在一定温度下样品表面上的氧化物层生长的发射率的变化。评估了在拟合质量上使用的参数数量的效果。比较了具有相同数量参数的发射率模型的配合质量。在氧化物膜的一定厚度下研究了温度的发射率的变化。三种近似模型用于探索具有氧化物层的温度和厚度的发射率的变化,其中两个被发现精确地再现发射率。在初始加热期间观察到发射率强的发射率强烈振荡,这是从氧化膜和来自基板的两个辐射之间的干扰效应产生的。

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