J. Neuhauser
Max Planck Society
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Featured researches published by J. Neuhauser.
Journal of Nuclear Materials | 1992
R. Schneider; D. Reiter; H.-P. Zehrfeld; Bastiaan J. Braams; Martine Baelmans; J. Geiger; H. Kastelewicz; J. Neuhauser; R. Wunderlich
The 2D multifluid edge code B2 coupled with the 3D neutral gas Monte Carlo code EIRENE is being used for edge interpretation and model validation on the axisymmetric poloidal divertor experiments ASDEX and ASDEX-Upgrade. For this purpose B2 was significantly improved especially by a fully implicit treatment of the topological cuts appearing in X-point configurations, and a reasonably accurate handling of inclined target plates. A fast, automatic grid generator has been developed, which allows direct implementation of experimental MHD equilibria into B2-EIRENE. Typical ASDEX and ASDEX-Upgrade simulations are presented and discussed.
Plasma Physics and Controlled Fusion | 1995
A. Herrmann; W. Junker; K Gunther; S Bosch; M. Kaufmann; J. Neuhauser; G. Pautasso; T. Richter; R. Schneider
A new thermography system with high time resolution was put into operation at ASDEX-Upgrade and is routinely used to determine the energy flux onto the lower diverter plates. The measurements allow the power deposition to be characterized during dynamic events such as ELMs and disruptions, as well as the asymmetry of the inboard/outboard power load. A power balance is set up even during single discharges and the losses are found to be fairly equal to the power input.
Nuclear Fusion | 1984
J. Neuhauser; Wolfgang Schneider; R. Wunderlich; K. Lackner
The impurity flow parallel to the magnetic field lines in a collisional tokamak scrape-off layer is numerically investigated. The rate equations are solved treating each ionization state as a test fluid which interacts with the given hydrogen background plasma via collisions and the ambipolar electric field. Results for typical impurities (O, Fe, He, etc.) show that collisional friction usually forces the impurities to flow nearly at hydrogen speed. Thermal forces, however, can become dominant locally for small Mach number and large temperature gradient (e.g. strong target recycling), causing impurity flow reversal and subsequent accumulation outside the recycling region. The criterion for flow reversal is roughly M <λi/λT where λi is the hydrogen ion mean free path and λT is the temperature gradient length. Self-sputtering at the target plates is calculated, showing the importance of fractional impurity acceleration in addition to the charge-statedependent electrostatic energy gain.
Nuclear Fusion | 1995
A. Kallenbach; R. Dux; V. Mertens; O. Gruber; G. Haas; M. Kaufmann; W. Poschenrieder; F. Ryter; H. Zohm; M. Alexander; K. Behringer; M. Bessenrodt-Weberpals; H.-S. Bosch; K. Büchl; A. Field; J. C. Fuchs; O. Gehre; A. Herrmann; S. Hirsch; W. Köppendörfer; K. Lackner; K. F. Mast; G. Neu; J. Neuhauser; S. D. Hempel; G. Raupp; K. Schonmann; A. Stäbler; K.-H. Steuer; O. Vollmer
Puffing of impurities (neon, argon) and deuterium gas in the main chamber is used to feedback control the total radiated power fraction and the divertor neutral particle density simultaneously in the ASDEX Upgrade tokamak. The variation of Psep=Pheat-Prad(core) by impurity radiation during H mode shows a similar effect on the ELM behaviour as that obtained by a change of the heating power. For radiated power fractions above 90%, the ELM amplitude becomes very small and detachment from the divertor plates occurs, whilst no degradation of the global energy confinement is observed (completely detached high confinement mode). Additional deuterium gas puffing is found to increase the radiated power per impurity ion in the plasma core owing to the combined effect of a higher particle recycling rate and a lower core penetration probability. The outer divertor chamber, which is closed for deuterium neutrals, builds up a high neutral pressure, the magnitude of which is determined by the balance of particle sources and pumping. For this particular situation, the effective pumping time of neon and argon is considerably reduced, to less than 0.3 s, mainly owing to an improved divertor retention capability. The radiation characteristics of discharges with a neon driven radiative mantle are modelled using a 1-D radial impurity transport code that has been coupled to a simple divertor model describing particle recycling and pumping. The results of simulations are in good agreement with experiment
Plasma Physics and Controlled Fusion | 1989
J. Neuhauser; M. Bessenrodt-Weberpals; Bastiaan J. Braams; A. Carlson; R Chodura; G. Fussmann; L. Giannone; G. Haas; G. Janeschitz; M. Kaufmann; M. Krech; K. Lackner; K. McCormick; D Meisel; E. R. Mueller; H. Murmann; H. Niedermeyer; W. Poschenrieder; J. Roth; A. Rudyi; U. Schneider; W. Schneider; G. Siller; A. Staebler
A survey of edge modeling and its application to running experiments is given with emphasis on poloidal divertors. The basic edge structure in axisymmetric and weakly perturbed tokamaks is first discussed. The ongoing modeling activities and the status of model validation are outlined. ASDEX data are mostly used for comparison, since sufficiently detailed and coherent edge measurements are not available in the literature for most experiments. Edge physics issues discussed in more detail are the basic model equations, parallel and perpendicular transport coefficients, thermoelectric effects, edge density limit and three-dimensional perturbations including magnetic field ergodization.
Nuclear Fusion | 1992
A. Stäbler; K. McCormick; V. Mertens; E. R. Müller; J. Neuhauser; H. Niedermeyer; K.-H. Steuer; H. Zohm; F. Dollinger; A. Eberhagen; G. Fussmann; O. Gehre; J. Gernhardt; T. Hartinger; J. Hofmann; E. Kakoulidis; M. Kaufmann; G. Kyriakakis; R.S. Lang; H. Murmann; W. Poschenrieder; F. Ryter; W. Sandmann; U. Schneider; G. Siller; F. X. Söldner; N. Tsois; O. Vollmer; F. Wagner
Density limit investigations on ASDEX have been performed under a variety of conditions: ohmically heated and neutral injection heated plasmas in H2, D2 and He have been studied in different divertor configurations, after various wall coating procedures, with gas puff and pellet fuelling, and in different confinement regimes with their characteristically different density profiles. A detailed description of the parametric dependence of the density limit, which in all cases is a disruptive limit, is given. This limit is shown to be a limit to the density at the plasma edge. Therefore, the highest densities corresponding to neRqa/Bt>30*1019 m-2.T-1 are obtained with centrally peaked ne profiles. Radiation from the main plasma at the density limit is always significantly below the total input power. The plasma disruption is due to an m=2 instability which for medium and high qa is preceded by one or more minor disruptions. In this range of qa, the disruptive instability is initiated by the occurrence of a Marfe on the high field side as a consequence of strong plasma cooling in this region. The duration of the Marfe increases with increasing distance between the plasma edge and the q=2 surface. After penetrating onto closed flux surfaces the Marfe leads to a current contraction and a subsequent destabilization of the m = 2 mode. In helium plasmas a strongly radiating, poloidally symmetric shell is observed before the density limit instead of a Marfe. An instantaneous destabilization of this mode is observed at low qa. Detailed measurements of plasma edge and divertor parameters close to the density limit indicate the development of a cold, dense divertor plasma before the disruption. Models describing the scrape-off layer and the divertor region predict an upper limit to the edge density at low divertor temperatures according to power balance considerations. Their relations to the experimental findings, especially the low field side cooling, ar
Journal of Nuclear Materials | 1984
J. Neuhauser; Wolfgang Schneider; R. Wunderlich; K. Lackner; K. Behringer
Abstract The impurity flow along magnetic field lines in a collisional tokamak scrape-off layer is numerically investigated using a testfluid approach. Transport perpendicular to the magnetic field is approximately included by a local loss time constant τ⊥. Results for various impurities and hydrogen background plasma parameters show the significance of thermal forces in the high recycling, subsonic flow regime. In this case, impurity flow reversal on “hot” field lines may cause impurity circulation in the scrape-off layer and, as a consequence, a stronger coupling between the main plasma and a separate pumping chamber than previously assumed.
Nuclear Fusion | 2008
J. Neuhauser; V. Bobkov; G. D. Conway; R. Dux; T. Eich; M. Garcia-Munoz; A. Herrmann; L. D. Horton; A. Kallenbach; S. Kalvin; G. Kocsis; B. Kurzan; P. T. Lang; M. Maraschek; H. W. Mueller; H. Murmann; R. Neu; A. G. Peeters; M. Reich; V. Rohde; A. Schmid; W. Suttrop; M. Tsalas; E. Wolfrum
In order to assess the contribution of edge localized modes (ELMs) to plasma–wall interaction in future fusion experiments like ITER, a sound experimental database for model validation and extrapolation, and, to be prepared for the unfavourable case, the development of tools for ELM mitigation are required. On ASDEX Upgrade a large amount of experimental information has been accumulated from various diagnostics on the structure and dynamics of natural as well as pellet induced ELMs, and on related wall effects. In this paper a survey of type-I ELM results is given first and recent progress is then described in detail. In between ELMs, strong mode activity is observed in a wide mode number and frequency range, specifically large amplitude (~20%) low frequency (several kilohertz) fluctuations. The initial dynamic ELM phase is dominated by the rapid growth of helical, low mode number structures rotating in the pedestal E × B direction, while the subsequent saturation and profile erosion phase is more complex and scenario dependent. Bursts of filaments ejected from the hot edge into the scrape-off layer are correlated with primary pedestal mode rotation. After partial edge profile collapse, a quiescent recovery phase is obtained despite substantial residual edge gradients. Pellet induced ELMs behave similarly to spontaneous ones, at least for the smallest pellets available so far.
Journal of Nuclear Materials | 1987
H. Verbeek; Asdex Team; G. Decker; H.-S. Bosch; H. Brocken; A. Eberhagen; G. Fussmann; O. Gehre; J. Gernhardt; G. v. Gierke; E. Glock; O. Gruber; G. Haas; J. Hofmann; A. Izvozchikov; G. Janeschitz; F. Karger; M. Keilhacker; O. Klüber; M. Kornherr; K. Lackner; M. Lenoci; G. Lisitano; F. Mast; H.-M. Mayer; K. McCormick; D. Meisel; V. Mertens; E. R. Müller; H. Murmann
Neutral particle fluxes onto the walls of ASDEX have been investigated using a time-of-flight (TOF) method. The energy distributions of the neutrals could be determined in the range of 10–1000 eV/amu. Ohmic divertor and limiter discharges with equal plasma currents and densities have been compared for He and D2. The He0 outflux at ∼2000 eV from He discharges is 110 of the corresponding D0 flux in D2 discharges. At lower energies this difference is much smaller. In all cases many more He neutrals were observed than was anticipated from the CX rate-coefficients for He2+. The impurity fluxes due to sputtering by the CX-neutrals show no significant difference for He and D2 discharges. For divertor discharges CX-sputtering can fully account for the Fe impurity content determined spectroscopically.
Journal of Nuclear Materials | 1995
H.-S. Bosch; J. Neuhauser; R. Schneider; A. Field; A. Herrmann; G. Lieder; W. Junker; C. S. Pitcher; D. Reiter; Bastiaan J. Braams
Abstract Due to the open field lines, the scrape-off layer and divertor region of tokamak plasmas is a complex, two-dimensional system, involving transport parallel and perpendicular to the magnetic field, as well as interaction of the plasma with surfaces and with the neutral gas. Therefore sophisticated two-dimensional codes are required to model the divertor and edge physics. In this paper, the B2-EIRENE code package is used to simulate the ASDEX-Upgrade scrape-off layer plasma and the neutral gas dynamics in a fully self-consistent way. Specific ASDEX-Upgrade discharges are modelled using the actual magnetic configuration and in-vessel components. Single fluid as well as multifluid calculations including self-consistent target and wall erosion of carbon are described. At given input power and bulk plasma radiation, typical divertor plasma profiles from Langmuir probes are fitted by varying the separatrix density and the transport coefficients. On the basis of such multifluid fits, spectroscopic divertor diagnostics are numerically modelled and compared with measured profiles, and reasonable agreement is found.