Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI

Extrinsic impurity seeding is planned for ITER to avoid high heat fluxes to the tungsten divertor targets. Nevertheless, excessive sputtering by impurities would lead to a reduction in fusion power output and divertor lifetime. Unlike today’s fusion devices, the entrainment of impurities is expected...

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Main Authors: Mark J.H. Cornelissen, Jordy W.M. Vernimmen, Jesse D.E. Verstappen, Erwin Zoethout, Ivo G.J. Classen, Job Beckers, Thomas W. Morgan
Format: Article
Language:English
Published: IOP Publishing 2024-01-01
Series:Nuclear Fusion
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Online Access:https://doi.org/10.1088/1741-4326/ad97ca
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author Mark J.H. Cornelissen
Jordy W.M. Vernimmen
Jesse D.E. Verstappen
Erwin Zoethout
Ivo G.J. Classen
Job Beckers
Thomas W. Morgan
author_facet Mark J.H. Cornelissen
Jordy W.M. Vernimmen
Jesse D.E. Verstappen
Erwin Zoethout
Ivo G.J. Classen
Job Beckers
Thomas W. Morgan
author_sort Mark J.H. Cornelissen
collection DOAJ
description Extrinsic impurity seeding is planned for ITER to avoid high heat fluxes to the tungsten divertor targets. Nevertheless, excessive sputtering by impurities would lead to a reduction in fusion power output and divertor lifetime. Unlike today’s fusion devices, the entrainment of impurities is expected to play an increasing role in ITER’s highly collisional near-surface plasma. Impurity entrainment refers to the acceleration of impurities with the plasma flow by collisional drag, leading to elevated impact energies. To investigate impurity entrainment under ITER-like divertor plasma conditions ( $n_{\mathrm{e}} \gt 2 \times 10^{20}$ m ^−3 , $T_{\mathrm{e}} \lt $ 5 eV), argon-seeded hydrogen plasmas were formed in the linear plasma generator Magnum-PSI. Doppler shifts in spatially-resolved emission profiles of argon (Ar II - 480.6 nm) and hydrogen (H $_\mathrm{\beta}$ - 486.1 nm) reveal the entrainment of seeded argon towards the upstream hydrogen velocity (∼9 cm from the surface), corresponding to ∼0.39 of the common-system sound speed. In addition, the sputtering yield of tungsten by argon bombardment for the argon-seeded hydrogen plasma was compared to a pure argon plasma by monitoring tungsten (W I - 400.9 nm) emission. These sputtering experiments reveal further entrainment of the argon impurities to ∼0.65 of the common-system sound speed at the sheath edge, leading to a large increase in their impact energy. Extrapolation of the Magnum-PSI results to ITER, using existing SOLPS-ITER simulations to determine the divertor plasma conditions, indicates more than an order of magnitude increase in gross erosion of the divertor targets due to impurity entrainment. However, the net erosion rate could still be kept under control if high re-deposition rates are achieved, which is treated in the companion paper (Cornelissen M.J.H. et al 2025 Nucl. Fusion 65 026008). The combination of a low sputtering threshold energy and high impact energy of impurities constrains the fine balance between radiative cooling with impurity seeding and avoiding extensive divertor erosion.
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spelling doaj-art-20257ff73ad8428b9895da2bb05436e92025-08-20T01:59:53ZengIOP PublishingNuclear Fusion0029-55152024-01-0165202600910.1088/1741-4326/ad97caErosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSIMark J.H. Cornelissen0https://orcid.org/0000-0001-7576-4628Jordy W.M. Vernimmen1https://orcid.org/0000-0003-2698-7459Jesse D.E. Verstappen2Erwin Zoethout3https://orcid.org/0000-0002-9012-6859Ivo G.J. Classen4https://orcid.org/0000-0001-8982-8856Job Beckers5https://orcid.org/0000-0001-6116-7013Thomas W. Morgan6https://orcid.org/0000-0002-5066-015XDepartment of Applied Physics, Eindhoven University of Technology , P.O. Box 513, Eindhoven, 5600 MB, Netherlands; DIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsDIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsDepartment of Applied Physics, Eindhoven University of Technology , P.O. Box 513, Eindhoven, 5600 MB, Netherlands; DIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsDIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsDIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsDepartment of Applied Physics, Eindhoven University of Technology , P.O. Box 513, Eindhoven, 5600 MB, NetherlandsDepartment of Applied Physics, Eindhoven University of Technology , P.O. Box 513, Eindhoven, 5600 MB, Netherlands; DIFFER—Dutch Institute for Fundamental Energy Research , De Zaale 20, Eindhoven, 5612 AJ, NetherlandsExtrinsic impurity seeding is planned for ITER to avoid high heat fluxes to the tungsten divertor targets. Nevertheless, excessive sputtering by impurities would lead to a reduction in fusion power output and divertor lifetime. Unlike today’s fusion devices, the entrainment of impurities is expected to play an increasing role in ITER’s highly collisional near-surface plasma. Impurity entrainment refers to the acceleration of impurities with the plasma flow by collisional drag, leading to elevated impact energies. To investigate impurity entrainment under ITER-like divertor plasma conditions ( $n_{\mathrm{e}} \gt 2 \times 10^{20}$ m ^−3 , $T_{\mathrm{e}} \lt $ 5 eV), argon-seeded hydrogen plasmas were formed in the linear plasma generator Magnum-PSI. Doppler shifts in spatially-resolved emission profiles of argon (Ar II - 480.6 nm) and hydrogen (H $_\mathrm{\beta}$ - 486.1 nm) reveal the entrainment of seeded argon towards the upstream hydrogen velocity (∼9 cm from the surface), corresponding to ∼0.39 of the common-system sound speed. In addition, the sputtering yield of tungsten by argon bombardment for the argon-seeded hydrogen plasma was compared to a pure argon plasma by monitoring tungsten (W I - 400.9 nm) emission. These sputtering experiments reveal further entrainment of the argon impurities to ∼0.65 of the common-system sound speed at the sheath edge, leading to a large increase in their impact energy. Extrapolation of the Magnum-PSI results to ITER, using existing SOLPS-ITER simulations to determine the divertor plasma conditions, indicates more than an order of magnitude increase in gross erosion of the divertor targets due to impurity entrainment. However, the net erosion rate could still be kept under control if high re-deposition rates are achieved, which is treated in the companion paper (Cornelissen M.J.H. et al 2025 Nucl. Fusion 65 026008). The combination of a low sputtering threshold energy and high impact energy of impurities constrains the fine balance between radiative cooling with impurity seeding and avoiding extensive divertor erosion.https://doi.org/10.1088/1741-4326/ad97caentrainmenterosiontungstenimpuritiesspectroscopyMagnum-PSI
spellingShingle Mark J.H. Cornelissen
Jordy W.M. Vernimmen
Jesse D.E. Verstappen
Erwin Zoethout
Ivo G.J. Classen
Job Beckers
Thomas W. Morgan
Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
Nuclear Fusion
entrainment
erosion
tungsten
impurities
spectroscopy
Magnum-PSI
title Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
title_full Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
title_fullStr Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
title_full_unstemmed Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
title_short Erosion enhancement by impurity entrainment in the highly collisional plasmas of Magnum-PSI
title_sort erosion enhancement by impurity entrainment in the highly collisional plasmas of magnum psi
topic entrainment
erosion
tungsten
impurities
spectroscopy
Magnum-PSI
url https://doi.org/10.1088/1741-4326/ad97ca
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