Physically principled reflection models applied to filtered camera imaging inversions in metal walled fusion machines.


Journal

The Review of scientific instruments
ISSN: 1089-7623
Titre abrégé: Rev Sci Instrum
Pays: United States
ID NLM: 0405571

Informations de publication

Date de publication:
Apr 2019
Historique:
entrez: 3 5 2019
pubmed: 3 5 2019
medline: 3 5 2019
Statut: ppublish

Résumé

Ray-tracing techniques are applied to filtered divertor imaging, a diagnostic that has long suffered from artifacts due to the polluting effect of reflected light in metal walled fusion machines. Physically realistic surface reflections were modeled using a Cook-Torrance micro-facet bi-directional reflection distribution function applied to a high resolution mesh of the vessel geometry. In the absence of gonioreflectometer measurements, a technique was developed to fit the free parameters of the Cook-Torrance model against images of the JET in-vessel light sources. By coupling this model with high fidelity plasma fluid simulations, photo-realistic renderings of a number of tokamak plasma emission scenarios were generated. Finally, a sensitivity matrix describing the optical coupling of a JET divertor camera and the emission profile of the plasma was obtained, including full reflection effects. These matrices are used to perform inversions on measured data and shown to reduce the level of artifacts in inverted emission profiles.

Identifiants

pubmed: 31043003
doi: 10.1063/1.5092781
doi:

Types de publication

Journal Article

Langues

eng

Pagination

043504

Auteurs

M Carr (M)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

A Meakins (A)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

S A Silburn (SA)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

J Karhunen (J)

Department of Applied Physics, Aalto University School of Science, P.O. Box 11100, FI-00076 Aalto, Finland.

M Bernert (M)

Max-Planck-Institut für Plasmaphysik, 85748 Garching, Germany.

C Bowman (C)

Department of Physics, York Plasma Institute, University of York, Heslington, York, United Kingdom.

A Callarelli (A)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

P Carvalho (P)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

C Giroud (C)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

J R Harrison (JR)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

S S Henderson (SS)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

A Huber (A)

Forschungszentrum Jülich GmbH, Institut für Energie-und Klimaforschung - Plasmaphysik, 52425 Jülich, Germany.

B Lipschultz (B)

Department of Physics, York Plasma Institute, University of York, Heslington, York, United Kingdom.

T Lunt (T)

Max-Planck-Institut für Plasmaphysik, 85748 Garching, Germany.

D Moulton (D)

UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom.

F Reimold (F)

Max-Planck-Institut für Plasmaphysik, Greifswald, Germany.
UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United KingdomDepartment of Applied Physics, Aalto University School of Science, P.O. Box 11100, FI-00076 Aalto, FinlandMax-Planck-Institut für Plasmaphysik, 85748 Garching, GermanyDepartment of Physics, York Plasma Institute, University of York, Heslington, York, United KingdomForschungszentrum Jülich GmbH, Institut für Energie-und Klimaforschung - Plasmaphysik, 52425 Jülich, GermanyMax-Planck-Institut für Plasmaphysik, Greifswald, Germany.
UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United KingdomDepartment of Applied Physics, Aalto University School of Science, P.O. Box 11100, FI-00076 Aalto, FinlandMax-Planck-Institut für Plasmaphysik, 85748 Garching, GermanyDepartment of Physics, York Plasma Institute, University of York, Heslington, York, United KingdomForschungszentrum Jülich GmbH, Institut für Energie-und Klimaforschung - Plasmaphysik, 52425 Jülich, GermanyMax-Planck-Institut für Plasmaphysik, Greifswald, Germany.
UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United KingdomDepartment of Applied Physics, Aalto University School of Science, P.O. Box 11100, FI-00076 Aalto, FinlandMax-Planck-Institut für Plasmaphysik, 85748 Garching, GermanyDepartment of Physics, York Plasma Institute, University of York, Heslington, York, United KingdomForschungszentrum Jülich GmbH, Institut für Energie-und Klimaforschung - Plasmaphysik, 52425 Jülich, GermanyMax-Planck-Institut für Plasmaphysik, Greifswald, Germany.
UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, United KingdomDepartment of Applied Physics, Aalto University School of Science, P.O. Box 11100, FI-00076 Aalto, FinlandMax-Planck-Institut für Plasmaphysik, 85748 Garching, GermanyDepartment of Physics, York Plasma Institute, University of York, Heslington, York, United KingdomForschungszentrum Jülich GmbH, Institut für Energie-und Klimaforschung - Plasmaphysik, 52425 Jülich, GermanyMax-Planck-Institut für Plasmaphysik, Greifswald, Germany.

Classifications MeSH