Observation of divertor currents during type-I ELMs on the DIII-D tokamak
In DIII-D, large currents flowing into the divertor floor during edge-localized modes (ELMs) have been measured by an array of shunt current resistors before an increase of heat flux is measured by IR thermography. The diagnostic consists of 40 tiles distributed in five concentric circles in the low...
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doaj-b3ab2edd22e54159b4010ed40b4ac7232020-11-24T22:00:51ZengElsevierNuclear Materials and Energy2352-17912019-01-0118222226Observation of divertor currents during type-I ELMs on the DIII-D tokamakM. Knolker0T.E. Evans1A. Wingen2A. Bortolon3C. Chrystal4F. Laggner5R.A. Moyer6R. Nazikian7H. Zohm8Ludwigs-Maximilians-Universitaet, Munich, Germany; Corresponding author.General Atomics, San Diego, CA, United StatesOak Ridge National Laboratory, Oak Ridge, TA, United StatesPrinceton Plasma Physics Laboratory, Princeton, NJ, United StatesGeneral Atomics, San Diego, CA, United StatesPrinceton Plasma Physics Laboratory, Princeton, NJ, United StatesUniversity of California at San Diego, San Diego, CA, United StatesPrinceton Plasma Physics Laboratory, Princeton, NJ, United StatesMaxPlanckInstitut für Plasmaphysik, Garching, GermanyIn DIII-D, large currents flowing into the divertor floor during edge-localized modes (ELMs) have been measured by an array of shunt current resistors before an increase of heat flux is measured by IR thermography. The diagnostic consists of 40 tiles distributed in five concentric circles in the lower divertor with sampling rates range between 50 and 500 kHz. Typically, the current measured by a single tile during an ELM can reach 500 A. This amounts to 5–25 kA flowing in the divertor tiles. The temporal evolution of the ELM currents shows a first phase with large amplitude oscillations, occurring before the heat flux increase measured by infrared thermography at the same location, lasting between 0.05 ms and 0.3 ms. A second phase follows where the time evolution of the divertor current mimics the evolution of the divertor heat flux. These currents could affect the plasma edge stability in the nonlinear ELM phase and provide a mechanism leading to explosive growth of edge stochasticity, the need of which and existence is predicted in contemporary nonlinear ELM simulations.http://www.sciencedirect.com/science/article/pii/S2352179118301315 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. Knolker T.E. Evans A. Wingen A. Bortolon C. Chrystal F. Laggner R.A. Moyer R. Nazikian H. Zohm |
spellingShingle |
M. Knolker T.E. Evans A. Wingen A. Bortolon C. Chrystal F. Laggner R.A. Moyer R. Nazikian H. Zohm Observation of divertor currents during type-I ELMs on the DIII-D tokamak Nuclear Materials and Energy |
author_facet |
M. Knolker T.E. Evans A. Wingen A. Bortolon C. Chrystal F. Laggner R.A. Moyer R. Nazikian H. Zohm |
author_sort |
M. Knolker |
title |
Observation of divertor currents during type-I ELMs on the DIII-D tokamak |
title_short |
Observation of divertor currents during type-I ELMs on the DIII-D tokamak |
title_full |
Observation of divertor currents during type-I ELMs on the DIII-D tokamak |
title_fullStr |
Observation of divertor currents during type-I ELMs on the DIII-D tokamak |
title_full_unstemmed |
Observation of divertor currents during type-I ELMs on the DIII-D tokamak |
title_sort |
observation of divertor currents during type-i elms on the diii-d tokamak |
publisher |
Elsevier |
series |
Nuclear Materials and Energy |
issn |
2352-1791 |
publishDate |
2019-01-01 |
description |
In DIII-D, large currents flowing into the divertor floor during edge-localized modes (ELMs) have been measured by an array of shunt current resistors before an increase of heat flux is measured by IR thermography. The diagnostic consists of 40 tiles distributed in five concentric circles in the lower divertor with sampling rates range between 50 and 500 kHz. Typically, the current measured by a single tile during an ELM can reach 500 A. This amounts to 5–25 kA flowing in the divertor tiles. The temporal evolution of the ELM currents shows a first phase with large amplitude oscillations, occurring before the heat flux increase measured by infrared thermography at the same location, lasting between 0.05 ms and 0.3 ms. A second phase follows where the time evolution of the divertor current mimics the evolution of the divertor heat flux. These currents could affect the plasma edge stability in the nonlinear ELM phase and provide a mechanism leading to explosive growth of edge stochasticity, the need of which and existence is predicted in contemporary nonlinear ELM simulations. |
url |
http://www.sciencedirect.com/science/article/pii/S2352179118301315 |
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