The compact radiative divertor at ASDEX Upgrade and its perspective for a fusion reactor
ORAL · Invited
Abstract
Experiments in the CRD configuration were conducted at ASDEX Upgrade: in a conventional divertor configuration the XPR was initiated by nitrogen seeding and then the plasma moved into the CRD configuration. Despite field line inclination angles below 0.2°, no glowing leading edge on the divertor tiles was observed. Infrared and bolometry measurements show that the heat load on the targets is dominated by radiation and not any more by heat conduction or convection of charged particles. The energy confinement remains at H-mode level while the XPR gives access to an ELM suppressed regime [2].
For a reactor the CRD has apparent advantages: The divertor design becomes much simpler and more volume is available for the confined plasma. While this already boosts the overall reactor performance, the current in the divertor magnetic field coils can also be reduced, easing their specification and increasing the plasma vertical stability. This is at the cost of requiring a higher plasma impurity content and strong control demands. Theory [3] indicates that the XPR, and with this the CRD, can be achieved more easily in a reactor scale device than in smaller devices and SOLPS simulations predict an excellent neutral divertor compression of this configuration.
As the benefits heavily outweigh the costs of this new configuration, the CRD might represent a game-changer for future reactor design.
[1] T. Lunt & M. Bernert et al 2023 PRL 130 145102
[2] M. Bernert et al 2021 NF 61 024001
[3] U. Stroth et al 2022 NF 62 076008
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Publication: T. Lunt & M. Bernert et al 2023 PRL 130 145102
Presenters
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Matthias Bernert
Max Planck Institute for Plasma Physics
Authors
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Matthias Bernert
Max Planck Institute for Plasma Physics
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Tilmann Lunt
Max-Planck-Institut für Plasmaphysik, Max Planck Institute for Plasma Physics, Garching, Germany
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Ou Pan
Max Planck Institute for Plasma Physics, Garching, Germany
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Dominik Brida
Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany, Max Planck Institute for Plasma Physics, Garching, Germany
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Pierre David
Max Planck Institute for Plasma Physics, Garching, Germany
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Michael Faitsch
Max Planck Institute for Plasma Physics, Max Planck Institute for Plasma Physics, Garching, Germany
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Andreas Redl
Universitá degli Studi della Tuscia, Viterbo, Italy
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Dirk Stieglitz
Max Planck Institute for Plasma Physics, Max Planck Institute for Plasma Physics, Garching, Germany
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Marco Wischmeier
Max-Planck-Institut für Plasmaphysik, Max Planck Institute for Plasma Physics, Garching, Germany
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Ulrich Stroth
Max Planck Institute for Plasma Physics, Garching, Germany