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Wang E, König R, Krychowiak M, Brezinsek S, Drews P, Gradic D, Jakubowski M, Kornejew P, Kremeyer T, Killer C, Liang Y, Neubauer O, Pandey A, Rudischhauser L, Sereda S, Schlisio G, Xu S. Radiation characteristics of detached divertor plasmas in W7-X. NUCLEAR MATERIALS AND ENERGY 2022. [DOI: 10.1016/j.nme.2022.101283] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/09/2022]
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Kobayashi T, Kobayashi M, Narushima Y, Suzuki Y, Watanabe KY, Mukai K, Hayashi Y. Self-Sustained Divertor Oscillation Driven by Magnetic Island Dynamics in Torus Plasma. PHYSICAL REVIEW LETTERS 2022; 128:085001. [PMID: 35275668 DOI: 10.1103/physrevlett.128.085001] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/21/2021] [Revised: 12/10/2021] [Accepted: 01/12/2022] [Indexed: 06/14/2023]
Abstract
A new type of self-sustained divertor oscillation is discovered in the Large Helical Device stellarator, where the peripheral plasma is detached from material diverters by means of externally applied perturbation fields. The divertor oscillation is found to be a self-regulation of an isolated magnetic field structure (the magnetic island) width induced by a drastic change in a poloidal inhomogeneity of the plasma radiation across the detachment-attachment transitions. A predator-prey model between the magnetic island width and a self-generated local plasma current (the bootstrap current) is introduced to describe the divertor oscillation, which successfully reproduces the experimental observations.
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Affiliation(s)
- T Kobayashi
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- The Graduate University for Advanced Studies, SOKENDAI, Toki 509-5292, Japan
| | - M Kobayashi
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- The Graduate University for Advanced Studies, SOKENDAI, Toki 509-5292, Japan
| | - Y Narushima
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- The Graduate University for Advanced Studies, SOKENDAI, Toki 509-5292, Japan
| | - Y Suzuki
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- The Graduate University for Advanced Studies, SOKENDAI, Toki 509-5292, Japan
- Graduate School of Advanced Science and Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan
| | - K Y Watanabe
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- Nagoya University, Graduate School of Engineering, Nagoya 464-8603, Japan
| | - K Mukai
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- The Graduate University for Advanced Studies, SOKENDAI, Toki 509-5292, Japan
| | - Y Hayashi
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
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Beidler CD, Smith HM, Alonso A, Andreeva T, Baldzuhn J, Beurskens MNA, Borchardt M, Bozhenkov SA, Brunner KJ, Damm H, Drevlak M, Ford OP, Fuchert G, Geiger J, Helander P, Hergenhahn U, Hirsch M, Höfel U, Kazakov YO, Kleiber R, Krychowiak M, Kwak S, Langenberg A, Laqua HP, Neuner U, Pablant NA, Pasch E, Pavone A, Pedersen TS, Rahbarnia K, Schilling J, Scott ER, Stange T, Svensson J, Thomsen H, Turkin Y, Warmer F, Wolf RC, Zhang D. Demonstration of reduced neoclassical energy transport in Wendelstein 7-X. Nature 2021; 596:221-226. [PMID: 34381232 PMCID: PMC8357633 DOI: 10.1038/s41586-021-03687-w] [Citation(s) in RCA: 10] [Impact Index Per Article: 3.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/30/2020] [Accepted: 06/02/2021] [Indexed: 02/07/2023]
Abstract
Research on magnetic confinement of high-temperature plasmas has the ultimate goal of harnessing nuclear fusion for the production of electricity. Although the tokamak1 is the leading toroidal magnetic-confinement concept, it is not without shortcomings and the fusion community has therefore also pursued alternative concepts such as the stellarator. Unlike axisymmetric tokamaks, stellarators possess a three-dimensional (3D) magnetic field geometry. The availability of this additional dimension opens up an extensive configuration space for computational optimization of both the field geometry itself and the current-carrying coils that produce it. Such an optimization was undertaken in designing Wendelstein 7-X (W7-X)2, a large helical-axis advanced stellarator (HELIAS), which began operation in 2015 at Greifswald, Germany. A major drawback of 3D magnetic field geometry, however, is that it introduces a strong temperature dependence into the stellarator's non-turbulent 'neoclassical' energy transport. Indeed, such energy losses will become prohibitive in high-temperature reactor plasmas unless a strong reduction of the geometrical factor associated with this transport can be achieved; such a reduction was therefore a principal goal of the design of W7-X. In spite of the modest heating power currently available, W7-X has already been able to achieve high-temperature plasma conditions during its 2017 and 2018 experimental campaigns, producing record values of the fusion triple product for such stellarator plasmas3,4. The triple product of plasma density, ion temperature and energy confinement time is used in fusion research as a figure of merit, as it must attain a certain threshold value before net-energy-producing operation of a reactor becomes possible1,5. Here we demonstrate that such record values provide evidence for reduced neoclassical energy transport in W7-X, as the plasma profiles that produced these results could not have been obtained in stellarators lacking a comparably high level of neoclassical optimization.
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Affiliation(s)
- C D Beidler
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany.
| | - H M Smith
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - A Alonso
- Laboratorio Nacional de Fusion, CIEMAT, Madrid, Spain
| | - T Andreeva
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - J Baldzuhn
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | | | - M Borchardt
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - S A Bozhenkov
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - K J Brunner
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - H Damm
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - M Drevlak
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - O P Ford
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - G Fuchert
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - J Geiger
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - P Helander
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - U Hergenhahn
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
- Fritz-Haber-Institut der Max-Planck-Gesellschaft, Berlin, Germany
| | - M Hirsch
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - U Höfel
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - Ye O Kazakov
- Laboratory for Plasma Physics (LPP), École royale militaire/Koninklijke Militaire School (ERM/KMS), Brussels, Belgium
| | - R Kleiber
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - M Krychowiak
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - S Kwak
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - A Langenberg
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - H P Laqua
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - U Neuner
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - N A Pablant
- Princeton Plasma Physics Laboratory, Princeton, NJ, USA
| | - E Pasch
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - A Pavone
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - T S Pedersen
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - K Rahbarnia
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - J Schilling
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - E R Scott
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - T Stange
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - J Svensson
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - H Thomsen
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - Y Turkin
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - F Warmer
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - R C Wolf
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
| | - D Zhang
- Max-Planck-Institut für Plasmaphysik, Greifswald, Germany
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Kwak S, Hergenhahn U, Höfel U, Krychowiak M, Pavone A, Svensson J, Ford O, König R, Bozhenkov S, Fuchert G, Pasch E, Brunner KJ, Knauer J, Kornejew P, Trimiño Mora H, Pedersen TS. Bayesian inference of spatially resolved Z eff profiles from line integrated bremsstrahlung spectra. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2021; 92:043505. [PMID: 34243367 DOI: 10.1063/5.0043777] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/11/2021] [Accepted: 03/12/2021] [Indexed: 06/13/2023]
Abstract
In nuclear fusion research, the effective ion charge Zeff, which characterizes the overall content of impurities, can be experimentally derived from the plasma electron-ion bremsstrahlung, given the electron density ne and temperature Te. At Wendelstein 7-X, a multichannel near-infrared spectrometer is installed to collect the plasma bremsstrahlung along 27 lines of sight covering more than half the plasma cross section, which provides information on Zeff over the entire plasma radius. To infer spatially resolved Zeff profiles, a Bayesian model is developed in the Minerva framework. Zeff, ne, and Te profiles are modeled as Gaussian processes, whose smoothness is determined by hyperparameters. These profiles are transformed to fields in Cartesian coordinates, given the poloidal magnetic flux surfaces calculated by the variational moments equilibrium code. Given all these physical quantities, the model predicts line-of-sight integrals of near-infrared bremsstrahlung spectra. The model includes the predictive (forward) models of the interferometer, Thomson scattering system, and visible and near-infrared spectrometers. Given the observations of all these diagnostics, the posterior probability distribution of Zeff profiles is calculated and shown as an inference solution. The smoothness (gradient) of the profiles is optimally chosen by Bayesian Occam's razor. Furthermore, wall reflections can significantly pollute the measurements of the plasma bremsstrahlung, which leads to over-estimation of Zeff values in the edge region. In the first results presented in this work, this problem does not appear, and the posterior samples of Zeff profiles are overall plausible and consistent with Zeff values inferred, given the data from the single-channel visible spectrometer.
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Affiliation(s)
- Sehyun Kwak
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - U Hergenhahn
- Fritz-Haber-Institut der Max-Planck-Gesellschaft, 14195 Berlin, Germany
| | - U Höfel
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - M Krychowiak
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - A Pavone
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - J Svensson
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - O Ford
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - R König
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - S Bozhenkov
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - G Fuchert
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - E Pasch
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - K J Brunner
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - J Knauer
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - P Kornejew
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | | | - T S Pedersen
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
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Rudischhauser L, Endler M, Höfel U, Hammond KC, Kallmeyer JP, Blackwell BD. The Langmuir probe system in the Wendelstein 7-X test divertor. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2020; 91:063505. [PMID: 32611053 DOI: 10.1063/1.5143013] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/23/2019] [Accepted: 05/28/2020] [Indexed: 06/11/2023]
Abstract
The design and evaluation of the Langmuir probe system used in the first divertor operation phase of Wendelstein 7-X is described. The probes are integrated into the target plates and have individually facetted surfaces to keep the angle of incidence of the magnetic field within an appropriate range for different magnetic configurations. Multiple models for the derivation of plasma parameters from current-voltage characteristics are introduced. These are analyzed with regard to their assumptions and limitations, generalized, and adapted to our use case. A detailed comparison is made to determine the most suitable model. It is found that the choice of model has a large impact, for example, resulting in a change in the inferred temperatures of up to a factor two. This evaluation is implemented in a Bayesian modeling framework and automated to allow for joint analysis with other diagnostics and a replacement of ad hoc assumptions. We rigorously treat parameter uncertainties, revealing strong correlations between them. General and flexible model formulations permit an expansion to additional effects.
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Affiliation(s)
- L Rudischhauser
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - M Endler
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - U Höfel
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - K C Hammond
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - J P Kallmeyer
- Max-Planck-Institut für Plasmaphysik, 17491 Greifswald, Germany
| | - B D Blackwell
- Australian National University, Canberra, ACT 2600, Australia
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