Preliminary design of an AXUV photodiode-based bolometer camera for MT-I spherical tokamak

•This paper presents the design and computational analysis of the bolometer camera for the MT-I spherical tokamak.The estimation of the line of sight (LOS) and field of view (FOV) of the AXUV system.•Optimization of the aperture by signal-to-noise ratio method and estimation of geometrical etendue.T...

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Veröffentlicht in:Fusion engineering and design 2024-06, Vol.203, p.114480, Article 114480
Hauptverfasser: Hussain, Azam, Zahid, Shah Zaib, Javed, M. Aqib, Khan, Riaz
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Sprache:eng
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Zusammenfassung:•This paper presents the design and computational analysis of the bolometer camera for the MT-I spherical tokamak.The estimation of the line of sight (LOS) and field of view (FOV) of the AXUV system.•Optimization of the aperture by signal-to-noise ratio method and estimation of geometrical etendue.The computation of plasma emissivity distribution using impurity densities and their cooling rates.•The computation of power incident on the photodiode array and signal-to-noise ratio (SNR). The MT-I is a spherical tokamak at the Pakistan Tokamak Plasma Research Institute, and has a major radius of 15 cm and a minor radius of 9 cm. This paper presents the design and computational analysis of the Absolute eXtreme Ultra-Violet (AXUV) photodiode-based bolometer camera, which will be used for the first time in the MT-I tokamak. The bolometer camera contains a single array of 16 AXUV photodiodes placed behind an aperture to compute the line of sight (LOS) and field of view (FOV) of the system. This array is located at the midplane of the vessel, which provides a radial resolution of about 16 mm. The individual FOV of each photodiode and the collective FOV of the array are 4.1° and ±34.5°, respectively. The impurity densities and their cooling rates for elements like carbon, oxygen, and iron are used to compute the plasma emissivity distribution, the power incident on the photodiode array, and signal-to-noise ratio (SNR) analysis. The analysis reveals that the radiated power loss is about 10 % of the ohmic heating input power. The geometrical etendue falls within the range of 2.2 × 10−5 to 3.2 × 10−5 Sr cm2. The bolometer exhibits a frequency response bandwidth of 10 kHz, and its temporal resolution is around 0.1 milliseconds.
ISSN:0920-3796
1873-7196
DOI:10.1016/j.fusengdes.2024.114480