Normal Spectral Emissivity Measurement of Molten Cu–Co Alloy Using an Electromagnetic Levitator Superimposed with a Static Magnetic Field

The normal spectral emissivity of molten Cu–Co alloy with different compositions was measured in the wavelength range of 780 nm to 920 nm and in the temperature range of 1430 K to 1770 K including the undercooled condition by an electromagnetic levitator superimposed with a static magnetic field. Th...

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Veröffentlicht in:International journal of thermophysics 2017-02, Vol.38 (2), p.1-9, Article 16
Hauptverfasser: Ueno, Shoya, Nakamura, Yuki, Sugioka, Ken-Ichi, Kubo, Masaki, Tsukada, Takao, Uchikoshi, Masahito, Fukuyama, Hiroyuki
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container_issue 2
container_start_page 1
container_title International journal of thermophysics
container_volume 38
creator Ueno, Shoya
Nakamura, Yuki
Sugioka, Ken-Ichi
Kubo, Masaki
Tsukada, Takao
Uchikoshi, Masahito
Fukuyama, Hiroyuki
description The normal spectral emissivity of molten Cu–Co alloy with different compositions was measured in the wavelength range of 780 nm to 920 nm and in the temperature range of 1430 K to 1770 K including the undercooled condition by an electromagnetic levitator superimposed with a static magnetic field. The emissivity was determined as the ratio of the radiance from a levitated molten Cu–Co droplet measured by a spectrometer to the radiance from a blackbody calculated by Planck’s law at a given temperature, where a static magnetic field of 2.5 T to 4.5 T was applied to the levitated droplet to suppress the surface oscillation and translational motion of the sample. We found little temperature dependence of the normal spectral emissivity of molten Cu–Co alloy. Concerning the composition dependence, the emissivity decreased markedly above 80 at%Cu and reached that of pure Cu, although its dependence was low between 20 at%Cu and 80 at%Cu. In addition, this composition dependence of the emissivity of molten Cu–Co alloy can be explained well by the Drude free-electron model.
doi_str_mv 10.1007/s10765-016-2136-z
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The emissivity was determined as the ratio of the radiance from a levitated molten Cu–Co droplet measured by a spectrometer to the radiance from a blackbody calculated by Planck’s law at a given temperature, where a static magnetic field of 2.5 T to 4.5 T was applied to the levitated droplet to suppress the surface oscillation and translational motion of the sample. We found little temperature dependence of the normal spectral emissivity of molten Cu–Co alloy. Concerning the composition dependence, the emissivity decreased markedly above 80 at%Cu and reached that of pure Cu, although its dependence was low between 20 at%Cu and 80 at%Cu. 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The emissivity was determined as the ratio of the radiance from a levitated molten Cu–Co droplet measured by a spectrometer to the radiance from a blackbody calculated by Planck’s law at a given temperature, where a static magnetic field of 2.5 T to 4.5 T was applied to the levitated droplet to suppress the surface oscillation and translational motion of the sample. We found little temperature dependence of the normal spectral emissivity of molten Cu–Co alloy. Concerning the composition dependence, the emissivity decreased markedly above 80 at%Cu and reached that of pure Cu, although its dependence was low between 20 at%Cu and 80 at%Cu. In addition, this composition dependence of the emissivity of molten Cu–Co alloy can be explained well by the Drude free-electron model.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10765-016-2136-z</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0003-2569-7863</orcidid></addata></record>
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subjects Blackbody
Classical Mechanics
Cobalt
Composition
Condensed Matter Physics
Copper base alloys
Droplets
Free electrons
Geophysics
Industrial Chemistry/Chemical Engineering
Magnetic fields
Physical Chemistry
Physics
Physics and Astronomy
Radiance
Spectra
Spectral emissivity
Temperature
Temperature dependence
Thermodynamics
Translational motion
title Normal Spectral Emissivity Measurement of Molten Cu–Co Alloy Using an Electromagnetic Levitator Superimposed with a Static Magnetic Field
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