8–12 Jul 2019
University of Milano-Bicocca UNIMIB
Europe/Rome timezone

P4.1099 Vacuum estimation of error field correction on ASDEX Upgrade

11 Jul 2019, 14:00
2h
Building U6 (University of Milano-Bicocca UNIMIB)

Building U6

University of Milano-Bicocca UNIMIB

Piazza dell’Ateneo Nuovo, 1 20126 Milan, Italy
MCF Poster P4

Speaker

D. Voltolina (EPS 2019)

Description

See the full abstract here:
http://ocs.ciemat.es/EPS2019ABS/pdf/P4.1099.pdf

A study of the vacuum magnetic field produced by the Poloidal Field (PF) coil system of ASDEX Upgrade is presented. In the model both coils and their power­supply feedthroughs are considered. The latter contribute to the error fields (EFs) that have already been observed and reported in [1, 2]. The effect on the B field due to PF coils, assumed to be perfectly axisymmetric, is addressed by analytical formulas, while a 1-D model is applied to feedthroughs [3]. The model is applied to a reference shot (#35352) for the computation of the normal component of B (i.e. B_n) projected on the q = 2 rational surface. The resulting EF pattern is located near the feedthroughs region, with a maximum value close to 0.25 mT. ASDEX Upgrade is equipped with a set of 16 in­vessel saddle coils [4], that can be used to minimize the effect of EFs on plasma discharges. A preliminary correction strategy of the non-axisymmetric field generated by feedthroughs is based on a Virtual Shell Approach, that is made up by 8 upper and 8 lower saddle loops built on the q = 2 surface. The matrix M_16×16 of the mutual inductances between active coils and virtual shell is computed numerically, such that I = M−1φ , where φ is the vector of the fluxes linked by the virtual shell loops and I stores the unknown currents needed for compensating those fluxes. A more detailed analysis is foreseen to include further possible sources of Efs (e.g. passive conductive structures, ferromagnetic tiles, tilting of PF coils). Moreover, MARS-F [5] can be used for calculations of plasma response to a prescribed m, n harmonic of the EF distribution, and a new correction strategy may be applied for reducing the resulting EF pattern.
[1] M. Maraschek, et al., Proc. 40th European Physical Society Conf. on Plasma Physics, P4.127 (Espoo, 2013) [2] V. Igochine, et.al., 2017 Nucl. Fusion 57, 116027 [3] J.D. Hanson, and S.P. Hirshman, Physics of Plasmas 9, 4410 (2002) [4] W. Suttrop, et al., Fusion Engineering and Design 84, 2 (2009) [5] Liu, Y.Q., et al., Physics of Plasmas 7, 3681 (2000) See the author list: H. Meyer, et al., 2017 Nucl. Fusion 57, 102014

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