In-situ study of the processes of damage to the tungsten surface under transient heat loads possible in ITER
Autor: | Dimitrii E. Cherepanov, G. G. Lazareva, A. A. Shoshin, Alexey S. Arakcheev, A.A. Kasatov, A. V. Burdakov, Leonid Vyacheslavov, I. V. Kandaurov, A. G. Maksimova, Vladimir A. Popov, A. A. Ruktuev, A. A. Vasilyev |
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Rok vydání: | 2021 |
Předmět: |
Nuclear and High Energy Physics
Materials science chemistry.chemical_element 02 engineering and technology Surface finish Bending Tungsten 021001 nanoscience & nanotechnology 01 natural sciences 010305 fluids & plasmas Nuclear Energy and Engineering chemistry Heat flux Residual stress 0103 physical sciences Surface roughness General Materials Science Surface layer Composite material 0210 nano-technology Intensity (heat transfer) |
Zdroj: | Journal of Nuclear Materials. 544:152669 |
ISSN: | 0022-3115 |
DOI: | 10.1016/j.jnucmat.2020.152669 |
Popis: | Experiments on the effect of fast heat loads on the surface of tungsten were carried out on the BETA facility at the Budker Institute. Tungsten samples were uniformly heated by an electron beam with a heat flux factor below the melting threshold. During and shortly after exposure, the 2D surface temperature distribution was measured, as well as the temperature history on selected surface areas. Active diagnostics using the scattering of CW laser light on a surface exposed by the electron beam allowed us to monitor the damage dynamics. At the heating stage, an increase in the surface roughness occurred, caused by inhomogeneous elastic and plastic deformations of the heated layer. As the cooling progressed, the residual plastic deformations remained. Simultaneously with the modification of the surface, bending of samples with a thickness of 3-4 mm occurred. The bending dynamics of the sample was measured by the intensity of a converging laser beam reflected from the back surface of the sample, polished to a mirror state. The residual sag due to bending increases with the heat load similarly as residual roughness of the front surface of the sample. These data, together with simultaneously measured temperature dynamics and the spatial heating profile, can provide an experimental basis for the numerical calculation of the residual stresses in the sample. The data obtained in situ were compared with those measured outside the vacuum chamber with X-ray diffraction, optical profiler, and optical interferometer. At the stage of cooling, after a sufficient intensity of heating, the second stage of damage took place — the cracking of the surface layer. The time before the start of this relatively fast process usually exceeded the time to achieve a DBTT by 1–4 orders of magnitude. |
Databáze: | OpenAIRE |
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