研究目的
To study the evolution of the mid-infrared emissivity of high-purity nickel during thermal oxidation and in its fully oxidized state, including the effects of magnetic phase transitions, to provide quantitative data for accurate radiative heat transfer calculations.
研究成果
The emissivity of nickel shows a change in slope at the Curie temperature due to magnetic phase transitions. During oxidation, the emissivity evolves with a mix of interferential and monotonic behaviors, leading to a non-trivial total normal emissivity evolution. The fully oxidized NiO exhibits emissivity characteristics influenced by phonon, two-phonon, and magnon interactions, with a non-linear temperature dependence. The study emphasizes the complexity of emissivity evolution and the need for accurate data in radiative heat transfer applications, highlighting the importance of substrate influence even in opaque layers.
研究不足
The study is limited to high-purity nickel and its oxide, which may not fully represent industrial alloys or other materials. The oxidation process was isothermal at 730°C, and results might vary under different conditions. Uncertainties in emissivity measurements increase at low temperatures and long wavelengths. The influence of surface roughness and other factors on emissivity is not extensively explored.
1:Experimental Design and Method Selection:
The study involved measuring the spectral emissivity of nickel and nickel oxide using a high-accuracy radiometer in controlled atmospheres (argon and air). The modified blacksur method was employed to avoid spurious reflections, and the radiometer was calibrated with a high-temperature blackbody and high-emissivity coating. Temperature was measured using thermocouples for Ni and the Christiansen wavelength method for NiO.
2:Sample Selection and Data Sources:
A high-purity (
3:999%) nickel sputtering target with a diameter of 50 mm and thickness of 2 mm was used. It was mechanically polished to achieve a specular surface with low roughness (Ra = 03 μm, Rq = 04 μm). The oxidized sample was characterized by X-ray diffraction, optical microscopy, and scanning electron microscopy. List of Experimental Equipment and Materials:
Equipment included a mechanical profilometer (Mitutoyo SJ201), X-ray diffractometer (X'Pert-Pro), optical microscope (Leica DM RXA), scanning electron microscope (FEG JEOL JSM-7000F), high-accuracy HAIRL radiometer, integrating sphere (Bruker A 562-G with Infragold coating), K-type thermocouples, and materials such as high-purity nickel, alumina powder for polishing, and argon gas.
4:Experimental Procedures and Operational Workflow:
The sample was polished and measured in argon from 200 to 800°C to establish baseline emissivity. It was then oxidized isothermally at 730°C in air for 33 days, with emissivity measured dynamically. After oxidation, the NiO layer was characterized, and emissivity of NiO was measured from below its Néel temperature to 850°C in argon. Data were collected and analyzed for spectral and total normal emissivity.
5:Data Analysis Methods:
Spectral emissivity data were integrated numerically with Planck function weighting to obtain total normal emissivity. Uncertainties were estimated, and results were compared with literature data. X-ray diffraction and microscopy were used for material characterization.
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