Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P2.1104 STRAHL modelling of impurity transport on Wendelstein 7-X during first divertor campaign

Jul 3, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Peter Traverso

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P2.1104.pdf STRAHL modelling of impurity transport on Wendelstein 7-X during first divertor campaign P. J. Traverso1, N. A. Pablant2, A. Langenberg3, R. Burhenn3, Th. Wegner3, D. Zhang3, B. Buttenschön3, B. Geiger3, D. A. Maurer1, J. Kring1, J. Schmitt1, and the W7-X Team 1 Auburn University, Auburn, AL, USA 2 Princeton Plasma Physics Laboratory, Princeton, NJ, USA 3 Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany In the first divertor operational phase (OP 1.2A) of Wendelstein 7-X, impurity transport experiments were performed with non-recycling materials via laser blow-off injection (LBO) [1]. The x-ray imaging spectrometer systems, HR-XIS [2,3] and XICS [4], were used to measure He-like spectra from the injected impurities in steady-state Helium discharges at various input ECRH heating powers and plasma densities. For these particular experiments the spatial and temporal emissivities from the mid-Z materials of either Titanium or Iron were measured, allowing for the estimation of the diffusion and convective velocity parameters for the respective measured charge state [5]. Utilizing the 1D transport code STRAHL [6], the spatial and temporal evolution of each impurity ionization charge state is modelled for assumed anomalous diffusion and convective velocity profiles. To match the experimentally measured emissivities, a chi-squared minimization is done on the experimental data by varying the input anomalous diffusion and convective velocity parameters for STRAHL. In addition a Gaussian process regression (GPR) [7] is used to improve and to better propagate the uncertainty estimates from the input electron temperature and density profiles in STRAHL to the modelled output diffusion and convective velocity parameters. [1] Th. Wegner et. al. HTPD conference San Diego (2018) [2] A. Langenberg, J. Svensson, H. Thomsen et al. Fusion Sci. Technol. 69 560-567 (2016) [3] G. Bertschinger, W. Biel, H. Jaegers, and O. Marchuk, Rev. Sci. Instrum. 75 3727 (2004) [4] N.A. Pablant, M. Bitter, R. Burhenn et al. 41st EPS conference on Plasma Physics Berlin (2014) [5] A. Langenberg, N.A. Pablant, O. Marchuk et al. Nucl. Fusion 57 086013 (2017) [6] R. Dux et al. IPP report 10/30 (2006) [7] M. A. Chilenski et al., Nucl. Fusion, 55, 2, 023012 (2015)

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