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首页> 外文期刊>Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics >Influence of roughness and composition on the total emissivity of tungsten, rhenium and tungsten-25% rhenium alloy at high temperature
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Influence of roughness and composition on the total emissivity of tungsten, rhenium and tungsten-25% rhenium alloy at high temperature

机译:高温下粗糙度和成分对钨,rh和25%tungsten钨合金总发射率的影响

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摘要

Measurements of the total directional and hemispherical emissivity of tungsten, rhenium and tungsten with 25% rhenium samples of various surface states was carried out in two wavelength ranges, 0.6-2.8 and 0.6-40 μm, from 1300 up to 2500 K in high vacuum. A clear trend was identified for the ratio of the 0.6-2.8 μm to the 0.6-40 μm hemispherical emissivity (assumed to be close to the true α/ε ratio, which is the ratio of the solar absorptivity a to the total emissivity s) as a function of the RMS roughness. This ratio is decreasing with increasing RMS roughness rapidly up to around 1 urn and then tends to sta bilize for higher roughness. It suggests that increasing the roughness, starting from a flat surface, will pro gressively give more weight to the long wavelength range emissivities in comparison to the short wavelength ones. Beside the RMS roughness, a sharp surface structure on a finer scale found on some samples also led to an additional decrease of the α/ε ratio, but these structures are not stable at high tem perature and disappear due to a natural high temperature smoothing. Finally our results also show that the α/ε ratio of rhenium is lower than the one of tungsten.
机译:使用25%samples样品的不同表面态的钨,rh和钨的总方向性和半球发射率的测量是在0.6-2.8和0.6-40μm的两个波长范围内(从1300到2500 K)在高真空下进行的。对于0.6-2.8μm与0.6-40μm的半球形发射率之比(假定接近于真实的α/ε比,即太阳吸收率a与总发射率s之比),存在明显的趋势。作为RMS粗糙度的函数。该比率随着RMS粗糙度的增加而迅速减小,直到1 um左右,然后趋于稳定以获得更高的粗糙度。这表明从平坦表面开始增加粗糙度,与短波长发射率相比,将逐渐增加长波长范围发射率的权重。除RMS粗糙度外,在一些样品上发现的较细尺度的尖锐表面结构还导致α/ε比的进一步降低,但这些结构在高温下不稳定,并由于自然的高温平滑而消失。最后,我们的结果还表明,the的α/ε比值低于钨。

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