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

O3.104 Energy confinement in the pellet-enforced high-density regime at ASDEX Upgrade

10 Jul 2019, 12:25
15m
Aula Magna, Building U6 (University of Milano-Bicocca UNIMIB)

Aula Magna, Building U6

University of Milano-Bicocca UNIMIB

Piazza dell’Ateneo Nuovo, 1 20126 Milan (Italy)
MCF MCF

Speaker

P.T. Lang (EPS 2019)

Description

See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.104.pdf

Operation in a future fusion reactor will aim to establish a high plasma core density n0 in order to harvest a maximum output power. Hence, for example the near term EU-DEMO1 concept foresees operation at n0 values at or even beyond 1.2 the Greenwald density nGw. Like for most envisaged reactor scenarios this approach assumes as well a confinement that can be achieved as predicted by the H98(y,2) scaling. This scaling predicts that the energy confinement time E increases with the line averaged electron density as 0.41. However, the data set employed for deriving this scaling contains very little input from the high density regime. This is due to the fact that a significant loss of confinement sets in when gas puff fuelling is applied, encountering the H-mode density limit at about 0.8 - 0.85 x nGw. Reliable access to the high density regime while sustaining good confinement is typically allocated to the injection of fuelling pellets, mm sized bodies formed of solid hydrogen. Accordingly, fuelling experiments proved H-mode operation at trans-Greenwald density, the achievable confinement however never showed the favourable ~ 0.41 correlation. In order to provide a better understanding of the confinement behaviour in this pellet generated high-density regime, a data base was created covering a wide range of experiments performed at the all-metal-wall tokamak ASDEX Upgrade. They include plasma scenarios run with and without ELM mitigation, with and without impurity seeding, the ITER base line configurations but also straightforward technical discharges for actuator tests. In total, the data base contains 598 time slices from 47 different discharges; ranging from 0.5 - 1.85 x nGw. As expected, data above 0.8 x nGw shows a rather poor correlation with the H98(y,2) predictions, which are significantly overestimating observed values. Much better agreement is found with the more sophisticated scaling H06 which predicts a roll-over to ~ 0 when approaching high densities. Efforts taken for performance enhancement by e.g. shaping or seeding result in a clear positive impact below 0.8 x nGw; however these improvements are quickly fading away with increasing until beyond 1.2 x nGw no visible improvements remain. In the pellet-enforced high-density regime, the achievable plasma confinement becomes virtually insensitive to measures usually found effective for low and moderate densities. Major excursions from this behaviour are only observed for cases when deterioration is caused by adversities like e.g. excessive edge fuelling, core impurity accumulation or strong mode activity.

This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 and 2019-2020 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission.

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